第 92 期·中文精讀

哈里·克利夫:粒子物理與大型強子對撞機

Harry Cliff: Particle Physics and the Large Hadron Collider

粒子物理學家介紹大型強子對撞機如何運作、希格斯玻色子的發現,以及標準模型之外的未解之謎。

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粒子物理學這個名字起得不好。

宇宙的基本成分壓根就不是粒子。真正鋪滿整個空間、無處不在的,是一種看不見摸不著、像流體一樣的東西,物理學家管它叫量子場。

哈里·克利夫(Harry Cliff)是劍橋大學的粒子物理學家,在大型強子對撞機上做 LHCb 實驗。他在倫敦皇家研究院的講臺上說,我們從小在教科書上看到的原子圖,那個中間一坨質子中子、外面幾個電子像小飛蟲繞圈的圖,誤導性極強。電子壓根不像繞著原子轉的小行星,它是一團彌散的、抖動的、像波一樣的東西。這件事從二十世紀初量子力學建立的時候就知道了,只是我們一直沿用“粒子”這個詞,因為很多時候它確實表現得像顆小彈珠。

場是什麼?

法拉第在十九世紀做過一個著名實驗。他把磁鐵放在一張紙下面,撒上鐵屑,鐵屑自動排成一道道弧線。那些弧線就是磁場的形狀,一種看不見的影響力被畫了出來。法拉第當年做實驗的地方,正是克利夫這次談話所在的這棟樓。

現代物理學的看法是:粒子,就是這些無處不在的場上面泛起的一點點漣漪。

我們身體本質上是由能量打的結組成的,這些結就存在於我們周圍那些看不見的東西里面。(哈里·克利夫)

一臺撞向真空的顯微鏡

大型強子對撞機(LHC)周長 27 公里,埋在日內瓦郊外鄉間地下 100 米處。克利夫說,你可以把它理解成一臺巨型顯微鏡,這個類比其實相當精確。

只不過它觀察的物件,是真空的結構。

為什麼要撞真空?因為真空裡並不空。拿希格斯場舉例,它是整個宇宙中唯一一個處處不為零的場。你跑到宇宙最荒涼的角落,拿個大盒子罩住,把電磁場測一遍,讀數基本是零,只剩一點量子漲落。希格斯場完全另一個樣子,整個空間都存著它的一份能量,就像空間本身有一個背景溫度。電子和夸克之所以有質量,就是因為它們跟這份能量發生了相互作用。

2012 年 LHC 發現希格斯玻色子,本質上是往這個場裡打出了一個漣漪。兩個質子以極高的能量對撞,能量足夠在希格斯場裡激起一處擾動,這處擾動就表現為一個希格斯玻色子。

玻色子本身沒那麼重要,重要的是場。發現玻色子,只是我們確認場存在的方法。

為什麼非修這麼大

粒子加速器只有兩種造法:環形和直線。環形的優勢是,粒子每繞一圈,你就能給它加一次速。

LHC 上有一段約 30 米長的裝置,裡面排著一串金屬盒子,盒子裡是頻率兩百萬伏特的振盪電場。電場時序調得極準:質子飛近時,它感受到的是吸引力;質子離開時,電場剛好翻轉成排斥,把它從另一頭推出去。每過一次,快一點。然後繞回來,再過一次。

束流由一團一團的粒子組成,克利夫形容它們像一群群蜜蜂。環上大約排著兩千個束團,如果你站在環上某一點數,每秒有 4000 萬個束團從你面前經過。加速電場的振盪頻率是幾百兆赫茲,比束團經過的頻率高得多,時序上必須嚴絲合縫。

那為什麼不能修小一點?

因為質子的速度已經到了光速的 99.9999991%。開快車過彎,你需要足夠的輪胎摩擦力,否則車會滑出去。粒子過彎靠的是磁場,磁場越強,彎道就能拐得越急。LHC 設計時用的已經是當時能造出來的最強磁鐵。這中間有個取捨:隧道越大,磁鐵可以越弱;隧道越小,磁鐵必須越強。

克利夫承認,這些問題如果去問工程師,對方大概會當場喊起來,因為真正的工程難度遠比“原理上不難”複雜得多。但原理層面確實就是這個賬。

比頭髮絲還細、三十釐米長的束團

束團的形狀挺特別:長約 30 釐米,比頭髮絲還細,橫截面直徑只有 12 微米。一個束團裡裝著一千億個質子。

兩束迎面對撞,真正撞上的可能只有十幾個。

所以你沒法讓單個粒子精確對撞單個粒子,只能靠機率。克利夫打了個比方:兩群鳥迎面飛過,如果鳥在群裡散得很開,撞上的機會很小;如果擠得密密麻麻,撞上的機會就大。所以要把束流壓得越細越好。

我問他這裡有多少軟體成分。他說這取決於你問哪一層,整個機器當然是計算機控制的,CERN 有個像 NASA 任務控制中心那樣的控制大廳,工程師坐在成排的工位前監控,因為機器執行時人不可能待在隧道里。

他講了一個 2008 年的故事。LHC 首次啟動,辦了一場盛大的釋出會和慶功宴。大約十天後,他們在做測試,隧道里發生了一次大爆炸,損毀了半公里長的機器。控制室裡的工程師看到滿屏報警開始變紅,第一反應是軟體出問題了,因為沒人相信真能出這麼嚴重的事故。

五分鐘講完二十世紀物理學

十九世紀末,人們對物質的基本看法是:物質由原子構成,原子不可分割、不可改變,每個化學元素對應一種原子。

1897 年,劍橋卡文迪許實驗室的實驗顯示,原子內部還有更小的東西,帶負電,後來被叫作電子。幾年後,盧瑟福證明原子中心有一個極小的核,帶正電。到 1910 年前後,我們在學校裡學的那種原子模型就成型了。

再往後,人們用放射性元素射出的 α 粒子當子彈去轟別的原子,把核裡的東西打了出來。先發現的是質子,帶正電,質量約是電子的兩千倍。大約十年後又發現了中子,不帶電。

到此為止,原子的三種基本成分齊了:核裡的質子和中子靠強力綁在一起,外面的電子靠電磁力被拉住。1932 年,物理學看起來乾淨漂亮,一切都很美好。

然後就出問題了。

雲室實驗讓人們第一次能給亞原子粒子“拍照”,看到它們的軌跡。人們用雲室研究宇宙射線,也就是從太空飛來撞進大氣層的粒子。結果發現了一大堆新東西。

其中一項收穫是反物質。狄拉克把量子力學和相對論結合起來,理論上預言了反電子的存在,也就是正電子。預言做出大約一年後,正電子就被實驗發現了。狄拉克大概是二十世紀除了愛因斯坦之外最聰明的物理學家,名氣卻小得多。

正電子遇到電子會發生什麼?兩者互相湮滅,質量全部轉化成能量,通常變成光子,也就是光。

接著,更多奇怪的粒子冒了出來。它們大多參與強力,有點像質子和中子,但顯然不是構成原子的材料。到 1960 年前後,這類粒子已經發現了一百多種,物理學家快把頭髮薅光了,因為物理學的全部追求就是簡化,而原本簡單的東西突然變得又亂又雜。

夸克:永遠拿不出來的積木

默裡·蓋爾曼(Murray Gell-Mann)注意到這些粒子之間存在對稱性。按特定方式排列,它們之間就有規律可循。他用對稱性預言了一些尚未被發現的粒子,後來果然在加速器上找到了。這說明那一百多種粒子並非一堆隨機的垃圾,底下壓著秩序。

1960 年代,蓋爾曼和喬治·茨威格(George Zweig)提出,這些規律之所以出現,是因為這些粒子本身由更小的東西組成,那東西叫夸克。

問題是,很長時間裡沒人相信夸克是真的。大家覺得那只是個理論上的方便工具,湊巧能擬合資料。大量實驗試圖把夸克從質子或中子中打出來,從來沒成功過。到今天也沒有。

真正說服人的證據來自加州斯坦福的三公里長直線加速器:一臺巨型電子槍,把接近光速的電子射向質子。結果發現,高能電子會從質子內部一些又小又硬的東西上彈開。這有點像給質子拍 X 光片,那些硬邦邦的東西就是夸克。質子內部有三個這樣的東西。

那為什麼把夸克拽不出來?

因為強力太強了。你可以把兩個夸克想象成被一根極強的彈簧連著。你拉,拉,拉,能量不斷注入這根“彈簧”。張力大到一定程度,彈簧啪地斷了,而斷口處注入的能量會立刻變成兩個新的夸克,分別掛在兩個斷頭上。你開始有兩個夸克,最後有四個。你永遠拿不出一個孤立的夸克,只會在這個過程中造出更多夸克。

所以夸克的存在,是透過散射角度推斷出來的,是透過這個模型能預言新粒子、能跟海量實驗資料吻合來確證的。它確實是真的,只是你沒法把它單獨拿出來看一眼。

質量從哪裡來

標準模型裡只有兩種粒子沒有質量:光子和膠子。膠子是強力的粒子形態,就像光子是電磁力的粒子形態。

其餘所有物質粒子,六個夸克、六個輕子(包括電子和它的兩個更重的版本,以及三種中微子),全都有質量。

弱力的傳遞粒子也有質量,而且非常大。W 加、W 減、Z 玻色子,質量是質子的 80 到 90 倍。最重的是頂夸克,大約是質子質量的 175 倍。

這帶來一個理論上的災難。六十年代,物理學家發現,如果在一套量子場論裡塞進帶質量的力場,計算會給出無窮大的結果。不只是力粒子,連電子有質量都是個問題。

希格斯的方案是:所有粒子本來都沒有質量,質量是後來“得到”的。

具體機制是引入一個新的場,也就是希格斯場。電子在希格斯場裡,場會在電子周圍聚攏,被電子吸引過去。這團聚集在電子周圍的場裡儲存的能量,就是我們測量到的電子的質量。

如果能把希格斯場關掉,自然界所有粒子都會變得沒有質量,以光速四處飛。(哈里·克利夫)

這個想法一出來,電磁力和弱力就能被統一成一個理論的兩個側面。七十年代中期寫成的電弱理論預言了四種新粒子:W 加、W 減、Z 玻色子和希格斯玻色子。1983 到 1984 年,前三者在 CERN 的一臺七公里加速器上被找到了。

所以從八十年代起,物理學界就很確信希格斯一定存在,這套理論結構少了它就不成立。

順便說一句,LHC 現在用的那條 27 公里隧道,原本是給上一代的“大型正負電子對撞機”準備的。那臺機器 1980 年代末 1990 年代初執行,主要貢獻是以極高精度研究 W 和 Z 粒子,把電弱理論驗證到很紮實的程度。1999 年它關機時,人們已經很確信:希格斯,或者非常像希格斯的某種東西,一定存在。

所以希格斯粒子的發現,從某個角度看只是“確認了顯然的事”。像一個拼圖,每一塊都拼好了,畫面很美,只剩中間一個缺口,你幾乎能確定那塊一定在某個地方。

真正有意思的地方在別處:希格斯粒子很古怪。它在標準模型裡與其他所有粒子都不同,理論上非常麻煩,也非常可疑。

一個被調到刁鑽位置的場

測量這個房間裡的電磁場,你會測到各種東西:光、微波、無線電波。跑到真正空無一物的遠方,用盒子罩住再測,電磁場基本歸零。

希格斯場的表現完全不同。它在任何地方都有一個非零的值。整個宇宙空間裡,希格斯場都存著一份能量。這份能量的精確數值,決定了電子和夸克的質量。

而這個數值必須調得極其精準,宇宙裡才能出現有意思的東西。

如果按樸素的方式算,希格斯場大概只有兩種可能的歸宿:要麼處處為零,那就是一個所有粒子都沒質量、以光速亂飛、永遠無法形成原子的宇宙;要麼它會暴漲到普朗克能標,也就是量子引力的能標。到那個量級,連電子都會重到塌縮成黑洞,宇宙由黑洞組成,跟我們熟悉的任何東西都無關。

要讓它落在中間那個恰好的值上,需要“精細調節”:你得仔細調整標準模型裡其他場和它們的性質,才能得到這個像金髮姑娘的粥一樣剛剛好的結果。

克利夫說,這件事讓人覺得心裡發毛,同行們很不喜歡它。

可能的解釋有兩種。一種是設計者,他不排除這種可能,但那不是科學上可檢驗的假設。另一種是多重宇宙:存在無數個宇宙,我們恰好處在能誕生生命的那一個裡。他提到李·斯莫林(Lee Smolin)的一種想法,宇宙誕生於黑洞內部,宇宙之間透過某種類似達爾文演化的機制繁衍,能產生更多黑洞的宇宙更容易留下後代。

作為實驗物理學家,克利夫的態度是:這些想法有意思,但檢驗不了,所以他不太往那個方向想。

超對稱:一場沒有開成的派對

第三條路不需要多重宇宙,也不需要誰來調引數。它叫超對稱。

超對稱把力粒子和物質粒子聯絡起來,是自然界裡我們尚未見過、但原則上可能存在的一類對稱性中最晚近的幾種之一。費米子(物質粒子)和玻色子(力粒子)各自都有超對稱伴侶。這些額外場的效應,恰好能抵消標準模型場對希格斯場的干擾,把希格斯場自然穩定在一個合理的數值上,不需要任何人工微調。

超對稱還有別的吸引力:它預言暗物質粒子,還可能讓強力與電弱力在某個能量上統一起來。

所以 LHC 啟動前,期待值非常高。邏輯很順:如果超對稱負責穩住希格斯場,那這些超對稱粒子的質量應該就在 LHC 能探測的能量範圍附近。你既然發現了希格斯,大機率也應該發現超對稱伴侶。

然後,什麼都沒有。

LHC 已經跑了十來年,沒有任何超對稱粒子,也沒有任何超出標準模型的新粒子被找到。

超對稱之外還有別的方案。還有額外維度的理論,還有把希格斯粒子看成複合粒子的思路。最老的一類是“藝彩”(Technicolor),把希格斯看作兩個強相互作用粒子的束縛態,有點像夸克之於質子。這類理論被 LHC 的希格斯發現排掉了很大一部分。現在還有“部分複合性”的思路,劍橋的一些同事在做,認為希格斯是某些強相互作用粒子的束縛態,標準模型裡那些更重的粒子(比如頂夸克)也是這些複合粒子的混合態。

這類方案還能順帶回答另一個大問題:為什麼物質粒子有三代?我們周圍的一切由第一代構成,電子、電子中微子、上夸克、下夸克,但宇宙裡還有第二、第三代複製,μ 子、頂夸克等等。這些重複的圖案從哪來,我們一無所知。

標準模型裡六種夸克、六種輕子排成的表,看起來真的有點像元素週期表:列與列之間,圖案在重複。週期表的規律來自原子內部有電子和核,那這張表的規律來自什麼?

不找大象,找腳印

LHC 環上有四個大探測器。ATLAS 和 CMS 是兩個通用探測器,各三千人,它們發現了希格斯,也在找超對稱和暗物質。

克利夫所在的 LHCb 走的是另一條路。它研究 B 夸克,也叫“美夸克”或“底夸克”,克利夫說他們偏愛“美”,因為聽起來更性感。

B 夸克的好處是產量極大。LHCb 能造出幾千億個,因此可以把它們的性質測到極精確。

想象你在叢林裡找大象。要麼你到處亂轉,指望撞上一隻,但整片叢林可能只有一頭象,撞上的機會很小。要麼你低頭看地面,找大象留下的腳印。(哈里·克利夫)

LHCb 就是找腳印的那批人。他們不直接造出新的量子場,去找那些場在已知粒子身上留下的痕跡。那些尚未被發現的大質量場,會影響 B 夸克的行為,讓它們衰變的方式與標準模型的預言出現細微偏差。

這個任務的工程細節很驚人。B 夸克的壽命在粒子世界裡算相當長:1.5 萬億分之一秒。希格斯玻色子的壽命大概只有萬億分之一的萬億分之一秒。所以 B 夸克在衰變前會飛出一小段距離,幾釐米。探測器要做的,是在幾百條從質子對撞點射出的軌跡中,找出兩三條指向另一個位置、偏離幾釐米的軌跡,那說明有個 B 粒子飛了一段才衰變。

LHCb 內層的矽探測器距束流只有 7 毫米。而束流本身的能量相當於一架大型客機起飛,足以熔化一噸銅。一個狂暴到極點的東西,旁邊貼著這片薄如蟬翼的矽片。

ATLAS 和 CMS 的話,克利夫說它們像洋蔥,一層套一層。最靠近束流管的是矽做的徑跡探測器,粒子穿過時產生電訊號,一串電點連起來就能重建軌跡。外面一層叫量能器,測粒子能量。最外層是 μ 子室,μ 子是電子的重版本,像高速子彈,能一直打到探測器最邊緣。

宇宙為什麼沒有把自己滅掉

整場談話裡最大的問題,出現在這裡。

大爆炸時,按標準模型算,產生的物質和反物質應該一樣多。因為在我們所有的對撞實驗裡,造出一個粒子,必然同時造出一個反粒子,兩者總是一起出現,也總是一起湮滅。我們從未發現過能只造物質、不造反物質的機制。

那麼宇宙膨脹冷卻,大爆炸後幾秒鐘,就會發生一場“大湮滅”:所有粒子和反粒子迎頭相撞,變成光。之後留下的宇宙,應該是一個只有光子的、又黑又空的宇宙。

但物質還在。你我都在。

你和我都是殘渣。我們身體裡的每一個粒子,都是大爆炸之後不久那場物質與反物質的浩大槍戰中的倖存者。宇宙誕生時產生的粒子,大約只有十億分之一活到了今天。(哈里·克利夫)

為什麼會有這十億分之一的盈餘?

可能跟希格斯場有關。早期宇宙中,希格斯場從零變成今天這個值,是一次相變。在那之前,宇宙是一鍋沒有質量粒子的熱等離子體。相變發生時,就像氣體變成水滴,宇宙裡開始出現一個個小氣泡,氣泡裡希格斯場有了今天的值,粒子獲得了質量。在某些模型裡,物質和反物質在這些氣泡壁上反彈的方式不同,就會產生數量上的不對稱。

另一種可能跟中微子有關:存在某些奇異型別的中微子,它們衰變時偏向於產生物質而不是反物質。

這些都還只是設想。目前沒有任何明確證據指向其中哪一種。這正是 LHCb 想做的事,也是若干中微子實驗想做的事。

三千人的實驗,沒有老闆

我問他,幾千個聰明人、帶著各自的自尊心,怎麼才能捏在一起幹成一件事。

他說,從科學家的角度講,原因其實簡單:所有人在那裡

他說,從科學家的角度講,原因其實簡單:所有人在那裡都是為了同一個理由,想知道宇宙由什麼構成、自然規律是什麼。大家朝著同一個方向使勁。

當然,競爭也很真實。你的合作者,同時也是你的競爭者,大家都是學者,各有各的學校,都想成為那個把最激動人心的測量結果發出來的人。於是就有一種古怪的狀態:一邊要搶地盤,一邊又必須通力合作把實驗跑起來。而且居然執行得相當好。

更古怪的是組織結構。ATLAS 三千人,名義上的負責人叫“發言人”,由合作組選舉產生。但他沒有真正的權力。他不能開除任何人,他不是任何人的老闆。克利夫的老闆是劍橋的一位教授,不是他所在實驗的負責人。實驗負責人也沒法告訴他該幹什麼。

一群各自為政、自己當自己老闆的獨立學者,靠共識、靠開會、靠反覆討論,把事情做成了。

他還提到一件有意思的事:麥肯錫這類管理諮詢公司十幾年前專門進駐過 CERN,想搞明白這種組織到底是怎麼運轉的。三千個沒有上下級關係的人,沒有一個可以下命令的中樞,專案卻按時推進。這套東西在管理學教科書裡找不到對應模型。

克利夫還糾正了一個印象:外界總覺得物理學家必須是天才。他說不是這樣,聰明當然要有一定門檻,但很多最成功的實驗物理學家未必是腦子最聰明的那些。這個領域裡最重要的技能之一,是跟別人一起工作、交換想法的能力,以及肯下苦功。常常是決心和另一套技能的組合,決定了一個人走多遠。

LHC 的立項本身就是一場馬拉松。七十年代末開始有人討論,之後花了二十五年遊說、籌款、說服,直到 2000 年代初才破土動工。克利夫 2008 年入行時機器已經基本建成,他說自己對當年那些推動專案的人懷有極大的敬意,因為那些人做的事情,遠比寫論文難。

下一代對撞機,和十四道天塹

近期最確定的是 LHC 的高亮度升級。這次升級不提能量,提的是資料量:每秒更多對撞。因為跑幾年之後會出現收益遞減,每年新增的資料在總量裡佔比越來越小,要讓靈敏度真正上臺階,資料率得提高一個數量級。LHCb 的整個探測器正在重建,目標就是能吃下這個速率。

這一步很關鍵,因為 LHCb 已經在 B 夸克衰變裡看到了一些異常。多個測量裡都出現了偏差,方向彼此一致,看起來像某種新量子場留下的跡象。目前還沒到能宣佈“發現了什麼”的統計門檻,但很多個測量裡的偏差方向彼此吻合,這就值得盯住。

如果這些異常是真的,那就意味著我們看到了某個量子場作用在 B 夸克上的尾巴。要確認它,光看腳印不夠,得直接把那個場的粒子造出來,這就需要一臺能量更高的新機器。

歐洲目前正在做未來發展戰略的更新,桌面上擺著幾個方案。一個是在現有 27 公里隧道里換上更強的磁鐵,把能量提上去。這個方案便宜、穩妥,但很多人不喜歡,因為它是個死衚衕:做完這一步,這條路就走到頭了。

第二個叫 CLIC,緊湊型直線對撞機,正負電子對撞,用新的加速技術縮短距離。仍然是公里級,但不是一百公里級。

第三個支援率最高,叫未來環形對撞機(Future Circular Collider,FCC)。在日內瓦地區地下挖一條 100 公里周長的隧道,這大概是當地地質條件下能塞進去的最大尺寸。它會從 LHC 底下穿過,繞過萊芒湖,兜到阿爾卑斯山腳下,一直到日內瓦盆地的邊緣。

路線分兩步。先往隧道里放一臺正負電子機器,大量生產希格斯玻色子,把它研究到極精確,看它會不會表現出理論沒預料到的行為。很久以後再把它拆掉,換成質子對撞機,也就是一臺大得多的 LHC,去直接尋找暗物質,或者復現早期宇宙那次相變,看物質和反物質的不對稱是怎麼產生的。

代價是時間。最樂觀的估計,這些機器在 2040 年之前都拿不出資料。研發、設計、還有政治上的說服工作,全都要花時間。

錢呢?LHC 花了幾十億,如果把各種開銷都算進去,比較合理的估計是一百到一百二十億歐元。FCC 整個專案大約三百億歐元,攤到從現在到本世紀末的半個世紀裡。

克利夫補充了一句,如果 CERN 不做別的事,這個專案理論上能塞進現有預算。這話聽起來像自我安慰,但確實反映了這類大科學專案的財務邏輯:它買的是一臺機器背後的五十年科學產出,由幾十個國家分攤。

還有一個更遙遠也更殘酷的限制。他算過一筆賬:LHC 的對撞能量是 14 萬億電子伏特,這已經能觸及希格斯粒子和弱力粒子的量級。而弦論那些東西真正顯現自身的能標,是普朗克能標,大約 10 的 18 次方吉電子伏特。兩者差著 15 個數量級上下。

換句話說,如果要靠今天的加速器技術達到那個能量,機器得有多大?克利夫的答案是,得繞著銀河系修一圈。這個數字本身就是對“終極理論”的一種判詞:就算那套理論是對的,它的大部分預言我們也幾乎永遠無法在實驗室裡檢驗。

一個戰後為了和平而建的組織

CERN 是歐洲核子研究組織(European Organization for Nuclear Research),1950 年代戰後成立。它的定位有點像一份科學版的馬歇爾計劃:把歐洲的科學界重新聚到一起,做和平用途的事。

四十年代,大量中歐科學家逃往美國,歐洲眼睜睜看著一場人才流失。把這些人重新聚攏起來,做一個不造炸彈、由好奇心驅動的專案,這是當時的初衷。

組織方式很特別。國家簽約成為成員國,每年按 GDP 的很小一個比例繳費。英國大概一年出一兩億英鎊。

克利夫說這是個漂亮的想法。在沒有戰爭的年代,一群國家真的坐下來合作,就為了做好科學。

每秒四千萬次的取捨

LHC 產生的資料量,如果全記下來,幾天之內就能塞滿全世界所有的計算機。所以絕大部分被丟掉了。

記錄下來的只有極小一部分,大概萬分之一量級。這個篩選發生在探測器上,實時進行,叫觸發器(trigger)。它每秒要做四千萬次判斷:這次對撞裡有沒有可能藏著希格斯玻色子或暗物質粒子?有,就留下;沒有,扔。

過去這些演算法的邏輯相對樸素,比如算一下粒子的動量和能量,設個閾值,超過就記下來。

現在的趨勢是把機器學習儘可能往前推。不僅推到“要不要留下這次資料”這一層,甚至推到更下面一層。原始資料是一堆數字訊號:某個通道看到東西了,某個通道沒看到。這些訊號要先被擬合成軌跡,算出粒子飛行的方向,才能交給上層演算法判斷。

如果能讓機器學習直接看最原始的訊號,在某種意義上像是讓它在一張三維影象上做模式識別,那收益可能很大。因為現在的觸發器為了趕時間,沒法把資訊完整處理出來,效率被迫打折。演算法聰明一點,就能在不新建任何硬體的情況下,記錄下更多有用的資料,把更多背景提前剔除掉。

克利夫說這才是讓他興奮的地方:不用等一臺新機器,就能憑空拿到增益。當然,還是要買很多新的 GPU 農場。

在這棟樓裡講物理

談話的地點是倫敦的皇家研究院(Royal Institution),兩百年前成立,最初的宗旨就是把科學傳播給公眾。它是世界上最早一批讓科學家來公開演講的地方。

漢弗萊·戴維當年就在這裡做演示。他發現了笑氣,也發現了電解法,口才極好,對著十九世紀初的倫敦市民表演實驗。法拉第也在這裡講過課,同時在地下室裡做那些關於電磁的著名實驗。

克利夫在這裡講過兩次。他最喜歡的一場叫“Beyond the Higgs”,在皇家研究院的 YouTube 頻道上能找到。

我問他怎麼準備。他說沒有方法論。同樣的內容講過很多遍,講著講著,哪些故事有效、哪些解釋能讓人聽懂,自然就浮出來了。他當學生時就去學校做科普講座,現在偶爾還做。甚至還試過單口喜劇,效果還行,雖然過程嚇人。

我對這些想法是真的感興趣、真的興奮,我就是想講出來。(哈里·克利夫)

他還提到一句費曼的話:我無法創造的東西,我就無法理解。

他說自己並不是特別聰明,所以為了弄懂一件事,必須把它拆到最基礎的部分。而把這個過程講給別人聽,反過來又幫他真正弄懂。

科學傳播對他來說是一種學習方式。要把一個概念講清楚,你必須死盯著它看,而這一看,常常就發現自己原來根本沒懂。

他正在寫一本書,昨天剛剛經歷了這種事:意識到自己其實沒真正理解本專業裡一個相當基礎的理論要點,只好花兩天時間翻教科書、重新推敲,好讓書裡的解釋儘量貼近理論的實際樣子。

理解的層次是一層套一層的。越懂,最後講出來的東西反而越簡單,越容易聽懂。費曼的講義之所以好懂,原因就在這裡。

但也有例外。有些想法只存在於數學裡,唯一的理解途徑是去讀個物理學博士。希格斯機制他就承認自己講不清楚,只能給出一個不誤導人的大致輪廓。

把宇宙攤開,只剩幾條規則

我問他物理學裡最美的想法是什麼。

他先給了一個具體的:自然界的力,在我們的理論裡是對稱性的產物。

這是他本科時接觸到的,當時覺得不可思議。你假設宇宙遵守某種對稱性,這種對稱性比立方體的旋轉抽象一些,但性質上類似,然後你會發現,為了讓理論成立,你必須引入一種具有電磁力性質的力。換一種對稱性,得到強力。再換一種,得到弱力。

這些相互作用似乎來自某個更深的對稱原理。也可能我們只是事後在方程裡認出了對稱性,但這件事本身足夠漂亮。

然後他講了更讓他困惑的一點。

如果你把自然規律攤開看,粒子之間在極小尺度上的相互作用其實非常簡單:靠力場互相彈開,沿極其簡單的路徑運動。就靠這麼幾條規則、這麼幾種粒子,居然長出了整個宇宙。

這個宇宙複雜到不可想象,裡面有你我,有地球,有恆星。恆星靠自身引力的能量把重元素煉出來,再拋灑到宇宙各處,成為別的東西的原料。這條故事線可以一路追回到大爆炸之後萬億分之一秒。我們身上的一切,最終的來源都是那幾條簡單規則。

從簡單規則里長出這樣的複雜性,我覺得非常神秘,也非常奇怪。(哈里·克利夫)

而且這甚至不是物理學家能處理的問題。物理學家的活兒是往下挖,找更基本的定律。可是從幾條基本定律和幾種粒子走到一個分子,就已經難到算不動了;從分子走到一個人,根本無從下手。

所以才有化學,才有生物學。每一層都有自己的語言,因為下一層的方程在這個尺度上已經沒法用了。

留給讀者的幾件事

  • 下次看到教科書上那個原子圖,記住它靠不住。電子不像繞核飛行的小行星,它是一團彌散的波。這個認知上的修正,比記住任何一條公式都重要,因為它決定了你怎麼理解“真空”和“粒子”這兩個詞。
  • 想弄懂一個複雜概念,試著把它講給一個完全不懂的人聽。克利夫的辦法就是這樣:講不清楚的地方,就是你還沒真懂的地方。這一條對寫文件、做彙報、帶新人同樣成立。
  • 看科學新聞時留意“腳印”和“大象”的區別。直接發現新粒子是撞見大象,發現測量值系統性偏離預言是看到腳印。後者更常見,也更需要耐心,因為從腳印到確認大象,往往要十年。
  • 評估一個基礎科學專案的成本,把時間尺度一起算。三百億歐元聽起來驚人,攤到五十年、幾十個國家,比的是這半個世紀裡能產出什麼,而非一次性花掉多少錢。
  • 想跟進 LHCb 那些 B 夸克衰變的異常,去查“B 介子衰變輕子普適性”相關的進展。如果這些偏差最終被證實,那會是標準模型之外第一次真正意義上的裂縫。
  • 如果你在組織一個跨團隊的大專案,可以研究一下 CERN 的合作組模式:負責人由選舉產生、沒有解僱權、靠共識和會議推進。它證明了一件事,權力集中並非大規模協作的必要條件,共同的興趣和長期目標能頂替它的位置。
文稿由本站用語音識別模型(基於官方釋出音訊)機器轉寫,可能有識別錯誤,人名與數字請以音訊為準。
[00:00:00] The following is a conversation with Harry Cliffe, a particle physicist at the University of Cambridge working on the Large Hadron Collider beauty experiment that specializes in investigating the slight differences between matter and antimatter by studying a type of particle called the beauty quark, or because in this way he's part of the group of physicists who are searching for the evidence of new particles that can answer some of the biggest questions in modern physics. He's also an exceptional communicator of science with some of the clearest and most captivating explanations of basic concepts in particle physicist that have ever heard. [00:00:39] So when I visited London, I knew I had to talk to him and we did this conversation at the Royal Institute Lecture Theatre, which has hosted lectures for over two centuries from some of the greatest scientists and science communicators in history for Michael Faraday to Carl Sagan. This conversation was recorded before the outbreak of the pandemic for everyone feeling the medical and psychological and financial burden of this crisis. I'm sending love your way. Stay strong. We're in this together. [00:01:09] We'll beat this thing. This is the artificial intelligence podcast. If you enjoy it, subscribe. I need to review it with five stars, an app, a podcast, supporter and patron, or simply connect with me on Twitter. Àlex Friedman spelled F.R. Idi Amin as usual. [00:01:25] I'll do a few minutes of ads now and never any ads in the middle that can break the flow of the conversation. I hope that works for you and doesn't hurt the listening experience. Quick summary of the ads to sponsors Express VPN and Cash App. Please consider supporting the podcast by getting Express VPN and Express VPN Dotcom Slash Lex Pod and downloading cache app and using collects podcast. 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This show, sponsored by Express VPN, get it at Express dot com slash Lux pod to get a discount and to support this podcast. I've been using Express Japan for many years. I love it. It's easy to use the big power button and your privacy is protected and if you like, you can make it look like your location is anywhere else in the world. [00:03:11] I might be in Boston now, but I can make it look like I'm in New York, London, Paris or anywhere else. This has a large number of obvious benefits, certainly it allows you to access international versions of streaming websites like the Japanese, Netflix or the U.K. who express VPN works on any device you can imagine. I use a Linux shell out of Bunta Windows Android, but is available everywhere else to once again get it and express VPN dot com slash Lux pod to get a discount and to support this podcast. [00:03:47] And now here's my conversation with Harry Cliff. Let's start with probably one of the coolest things that human beings have ever created, the Large Hadron Collider LHC, what is it? How does it work? OK, so essentially this gigantic 27 kilometer circumference particle accelerators, this big ring buried under 100 meters underneath the surface in the countryside, just outside Geneva in Switzerland. And really what it's for ultimately is to try to understand what are the basic building blocks of the universe. [00:04:38] So you can think of it in a way as like a gigantic microscope. And the analogy is actually fairly precise. So gigantic microscope effectively, except as a microscope that looks at the structure of the vacuum in order for this kind of thing to study particles which are microscopic entities, it has to be huge, gigantic microscope. [00:05:02] So what do you mean by studying vacuum? [00:05:05] Okay, so I mean, it's a particle physics as as a field is kind of badly named in a way, because particles are not the fundamental ingredients of the universe. They're not fundamental at all. So the things that we believe are the real building blocks of the universe are objects, invisible fluid like objects called quantum fields. So these are fields like like the magnetic field around a magnet that exists everywhere in space that always there. In fact, actually, it's funny that we're in the wrong institution because this is where the idea of the field was effectively invented by Michael Faraday doing experiments with magnets and coils of wire. [00:05:40] So he noticed that, you know, if it's a very famous experiment that he did where he got a magnet and put it on top of it, a piece of paper, and then sprinkled iron filings and he found the iron filings arranged themselves into these kind of loops, which was actually mapping out the invisible influence of this magnetic field, which is the thing, you know, we've all experienced we've all felt held a magnet and or two poles, the magnet put them together and felt this thing was force pushing back. [00:06:05] So these are real physical objects. And the way we think of particles in modern physics is that they are essentially little vibrations, little ripples in these otherwise invisible fields that are everywhere. [00:06:18] They fill the whole universe. You know, I don't apologise perhaps for the ridiculous question. Are you comfortable with the idea of the fundamental nature of our reality being fields'? Because to me, particles, you know, a bunch of different building blocks makes more sense, sort of intellectually, sort of visually, like it seems to I seem to be able to visualize the kind of idea easier. Yeah. [00:06:45] Are you comfortable psychologically with the idea that the basic building block is not a block but a field? [00:06:52] I think it's I think it's quite a magical idea. I find it quite appealing. And it's well, it comes from a misunderstanding of what particles are so like when you when we do science at school and we draw a picture of an atom, you draw like, you know, a nucleus with some protons and neutrons, these little spheres in the middle. And then you have some electrons that are like little flies flying around the atom. And that is completely misleading. [00:07:13] Picture of what an atom is like is nothing like the electron is not like a little planet orbiting the atom. It's this spread out wibbly wobbly, wavelike thing. And we know we've known that since, you know, the early 20th century thanks to quantum mechanics. So when we carry on using this word particle, because sometimes we do experiments, particles do behave like their little marbles or little bullets, you know, so the LHC, when we collide particles together, you'll get you know, you get like hundreds of particles all flying out through the detector and they all take a trajectory. [00:07:44] And you can see from the detector where they've gone and they look like their little bullet. [00:07:48] So they behave that way, you know, a lot of the time. But when you really study them carefully, you'll see that they are not little spheres. They are these ethereal disturbances in in these underlying fields. So this is this is really how we think nature is, which is surprising, but also, I think, kind of magic. So we are our bodies are basically made up of like little knots of energy in these invisible objects all around us. [00:08:18] And what is the story of the vacuum when it comes to the LHC? So why did you mention the word vacuum? [00:08:26] Okay, so if we just if we go back to the physics, we do know. So atoms are made of electrons, which were discovered 100 or so years ago. And then in the nucleus of the atom, you have two other types of particles. There's an up something called an up clock and a down quark. And those three particles make up every atom in the universe. [00:08:44] So we think of these as ripples in field. So there is something called the electron field. And every electron in the universe is a ripple moving about in this electron field. So the electron field is all around us. We can't see it. But every electron in our body is a little ripple in this thing that's there all the time and the quark feels the same. So there's an up quark field and an up quark is literally up quark field and the down quark is a little. [00:09:08] In something else called the down quark field, so these fields are always there. Now, there are potentially we know about a certain number of fields in what we call the standard model of particle physics. The most recent one we discovered was the Higgs field. And the way we discovered the Higgs field was to make a little ripple in it. So what the LHC did, it fired two protons into each other very, very hard with enough energy that you could create a disturbance in this Higgs field. [00:09:35] And that's what shows up as what we call the Higgs boson. So this particle that everyone's going on about eight or so years ago is proof. Really the particle in itself is I mean, it's interesting. But the thing is really interesting is the field, because it's the Higgs field that we believe is the reason that electrons and quarks have mass and it's that invisible field that's always there that gives mass to the particles. [00:09:59] The Higgs boson is just our way of checking. It's there basically. [00:10:03] And so the Large Hadron Collider, in order to get that ripple in the Higgs field, you know, it requires a huge amount of energy. Yes. So that's why this huge that's why size matters here. So maybe there's a million questions here. But let's backtrack. Why does size matter in the context of a heck of particle collider? So why does bigger allow you for higher energy collisions? [00:10:32] Right. So the reason, well, is kind of simple, really, which is that there are two types of particle accelerator that you can build. One is circular, which is like the LHC. The other is a great long line. So the advantage of a circular machine is that you can send particles around a ring and you can give them a kick every time they go round. So imagine you have a is actually a bit of the LHC that's about only 30 metres long, where you have a bunch of metal boxes which have oscillating two million volt electric fields inside them, which are timed so that when a proton goes through one of these boxes, the field it sees as it approaches is attractive. [00:11:05] Then as it leaves the box, it flips and becomes repulsive and the person gets attracted and kicked out the other side. So it gets a bit faster. So you send it, then you send it back round again. [00:11:14] And it's incredible, like the timing of the synchronization where it really. Yeah, yeah, yeah. That's I think there's going to be a multiplicative effect. [00:11:22] And the question is, OK, let me just take that attention for a second. The orchestration of that, is that fundamentally a hardware problem or a software problem? [00:11:34] Like what? How do you get that? [00:11:37] I mean, I say first of all, say I'm not an engineer. So the guy is I did not build the LHC so that people much, much better at this stuff than I could for sure. [00:11:44] But maybe but from your sort of intuition, from the the echoes of what you understand, you heard of how is design, what's your sense, how what's the engineering aspects of the acceleration but is not challenging. [00:12:02] OK, OK. There are always challenges of everything. But basically you have these the beams that go round the LHC, the beams of particles are divided into little bunches. So they're called debris like swarms of bees, if you like. And there are around I think it's something of the order. Two thousand bunches spaced around the ring. And they if you if you were given point on the ring counting bunches, you get 40 million bunches passing you every second. [00:12:28] So they come in like, you know, like cars going past in a very fast motorway. So you need to have your electric field that you're using to accelerate the particles. That needs to be timed so that as a bunch of protons arrives, it's got the right sign to attract them and then flips at the right moment. [00:12:44] But I think the voltage in those boxes oscillates at hundreds of megahertz. So the beams that like 40 megahertz is oscillating much more quickly than the beam. So I think, you know, it's difficult engineering, but in principle it's not, you know, a really serious challenge. [00:12:58] The bigger problem is probably engineers like screaming at you right now, probably. So in terms of coming back to this thing, why is it so big? Well, the reason is you want to get the particles through that accelerating element over and over again. So you want to bring them back round. That's why it's round. The question is why couldn't you make it smaller? Well, the basic answer is that these particles are going unbelievably quickly. [00:13:20] So they travel at ninety nine point nine nine nine nine nine nine one percent of the speed of light in the LHC. And if you think about C driving your car around the corner, a high speed, if you go fast, you need a very you need a lot of friction in the tires to make sure you don't slide off the road. [00:13:38] So the the limiting factor is how powerful a magnet can you make? Because it's what we do is the magnets are used to bend the particles round the ring. And essentially the LHC, when it was designed, was designed with the most powerful magnets that could conceivably be built at the time. And so that's kind of limiting factors. [00:13:57] If you wanted to make the machines smaller, that means a tighter band. You need to have a more powerful magnet. So it's this toss up between how strong your magnets versus how big a tunnel can you afford. The bigger the tunnel, the weaker the magnets. B, the smaller the tunnel, the stronger they've got to be. OK, so maybe can we backtrack that a model and say what kind of particles there are, period? And maybe the history of kind of assembling that, the standard model of physics and then how that leads up to the hopes and dreams and the accomplishments of the Large Hadron Collider. [00:14:29] Yeah, sure. OK, so all of 20th century physics in like five minutes. Yeah, please. OK, so OK, the story really begins properly. [00:14:38] End of the 19th century. [00:14:39] The basic view of matter is that matter is made of atoms and the atoms are indestructible, immutable little spheres like the things we were talking about. [00:14:48] They don't really exist. And there's one atom for every chemical element. So it's an atom for hydrogen, for helium, for carbon, for iron, etc.. And they're all different than in 1897. Experiments done at the Cavendish Laboratory in Cambridge, where I'm still where I'm based, show that there are actually smaller particles inside the atom, which eventually became known as electrons. These are these negatively charged things that go round the outside a few years later. And it's Rutherfords, very famous. [00:15:14] Nuclear is one of the pioneers of nuclear physics, shows that the atom has a tiny nugget in the center, which we call the nucleus, which is a positively charged object. So then by like 1910 11, we have this model of the atom that we learn in school, which is you've got a nucleus, electrons go round it. [00:15:30] Fast forward, you know, a few years the nucleus, people start doing experiments with radioactivity where they use alpha particles that are spat out of radioactive elements as as bullets and they fire them other atoms. And by banging things into each other, they see that they can knock bits out of the nucleus. So these things come out called protons, first of all, which are positively charged particles about 2000 times heavier than the electron. And then 10 years later, more or less a neutral particle is discovered called a neutron. [00:16:00] So those are the three basic building blocks of atoms. You have protons and neutrons in the nucleus that are stuck together by something called a strong force, the strong nuclear force. And you have electrons in orbit around that held in by the electromagnetic force, which is one of the forces of nature. That's sort of where we get to by like 1932, more or less. [00:16:21] Then what happens is physics is nice and neat. In 1932, everything is great. We've got three particles in all the atoms are made of. That's fine. But then cloud chamber experiments. These are devices that can be used to the first devices capable of imaging subatomic particles. So you can see their tracks and they're used to study cosmic rays, particles that come from outer space and bang into the atmosphere. [00:16:42] And in these experiments, people start to see a whole lot of new particles. So they discover, for one thing, antimatter, which is the source of a mirror image of the particles. So we discover that there's also, as well as the negatively charged electron, there's something called a positron, which is a positively charged version of the electron. And there's an antiproton which is negatively charged, and then a whole load of other weird particles start to get discovered and no one really knows what they are. [00:17:05] This is known as the zoo of particles. Are these discoveries not the first theoretical discoveries or the discoveries in an experiment? So like. Well, yeah. What's the process of discovery for these early sets of it is a mixture. [00:17:20] I mean, the early stuff around the atom is really experimentally driven. It's not based on some theory. It's exploration in the lab using equipment. So it's really people just figuring out getting hands on with the phenomena of figuring out what these things are. And the theory comes a bit later that there is that's not always the case. So in the discovery of the anti electron, the positron that was predicted from quantum mechanics and relativity by a very clever theoretical physicist called Paul Dirac, who was probably the second brightest, you know, physicist of the 20th century, apart from Einstein, isn't as well anywhere near as well known. [00:17:53] So he predicted the existence of the anti electron from basically a combination of the theories of quantum mechanics and relativity. And it was discovered about a year after he made that prediction. [00:18:02] What happens when an electron meets a positron? They annihilate each other. So if you when you bring a particle into antiparticle together, they they react well, they react. They just wipe each other out and they turn their masses turned into energy, usually in the form of photons. So you get light produced. [00:18:20] So when you have that kind of situation, why why does the universe exist at all? If there's matter in any matter? Oh, God. Now we're getting into really big questions. [00:18:29] So you want to go there now? [00:18:32] That's maybe go there later. That's because I mean, that is a very big question. Yeah. Let's let's let's take it slow with the standard model. So, OK, so there's this matter and antimatter in the 30s, so what else. [00:18:46] So matter and antimatter and then a load of new particles start turning up in these cosmic ray experiments, first of all. And they don't seem to be particles that make up atoms. There's something else. They all mostly interact with a strong nuclear force. So they're a bit like protons and neutrons and buy in the 1960s in America particularly, but also in Europe and. Russia scientists, scientist, particle particle accelerator. So these are the forerunners of the LHC is a big ring shaped machines that were, you know, hundreds of meters long, which in those days was enormous in most physics. [00:19:18] Up until that point had been done in labs, in universities with small bits of kit. So this is a big change. And when these accelerators are built, they start to find they can produce even more of these particles. So I don't know the exact numbers, but by around 1960, there are over 100 of these things that have been discovered and physicists are kind of tearing the hair out because physics is all about simplification. And suddenly what was simple has become messy and complicated. [00:19:45] And everyone sort of wants to understand what's going on as a quick kind of aside and probably really dumb question. [00:19:51] But how is it possible to take something like a like a photon or an electron and be able to control it enough, like to be able to do a controlled experiment where you collide against something else? [00:20:08] Is that is that this seems like an exceptionally difficult engineering challenge because you mentioned vacuum tubes. [00:20:16] So you basically want to remove every other distraction and really focus on this collision. How difficult of an engineering challenge that just to get a sense and it's very hard. I mean, in the early days, particularly when the first accelerators are being built in 1932, Ernest Lawrence builds the first what we call a cyclotron, which is like a little salary to this big or so. There's another one, that big, tiny little thing. Yeah. I mean, so most of the first accelerators were what we call fixed target experiments. [00:20:47] So you had a ring. You accelerate particles around the ring and then you fire them out the side into some target. So that makes the kind of the colliding bit is relatively straightforward. Could use fire, whatever it is you want to fire. The hard bit is the steering, the beams with the magnetic fields getting, you know, strong enough electric fields to accelerate them, all that kind of stuff. The first colliders where you have two beams colliding head on, that comes later. [00:21:13] And I don't think it's done until maybe the 1980s. I'm not entirely not entirely sure, but it is much harder problem. [00:21:22] That's crazy because it's like perfectly the attempt to hit each other. And we're talking about what scale? [00:21:30] What's the I mean, the temporal thing is a giant mess, but the spacially like the size. Mm. Is tiny. What's give you a sense that the LHC beams the cross-sectional diameter is that I think around a dozen or so microns. [00:21:49] So you know ten, ten millions of a of a meter and a beam. [00:21:54] So just to clarify, a beam contains how many is it the bunches that you mentioned. Yeah. Multiple partners is just one part. Oh no, no. The bunches contain say 100 billion protons each. So a bunch is is not rebundle shaped it. They're actually quite long. They're like 30 centimetres long but thinner than a human hair. So like very, very narrow, long sort of objects. Those are the things. So what happens in the LHC is you steer the beams so that they cross in the middle of the detector. [00:22:23] So they basically have these swarms of protons that are flying through each other. [00:22:27] And most of the you have 100 billion coming one way, billion another way, maybe ten of them will hit each other. [00:22:34] Okay, so this is a lot more sense. That's nice. You're trying to use sort of it's a probabilistically you're not you can't make a single particle collide with a single. [00:22:43] Yeah. So that's not an efficient way to do it. You'd be waiting a very long time to get anything. Yeah. [00:22:47] So you're basically right. You're relying on probability to be some fraction of them are going to collide and then, you know, which is it? It's a it's a swarm of the same kind of particle. [00:23:01] So it doesn't matter which ones each other. Exactly. I mean, that that's not to say it's not hard. You've got to one of the challenges to make the collisions work is you have to squash these beams to very, very basically the narrower they are, the better, because the higher the chances of them colliding. If you think about two flocks of birds flying through each other, the birds are far apart in the flocks. There's not much chance that they'll collide if they're all flying densely together and they're much more likely to collide with each other. [00:23:25] So that's the sort of problem. It's tuning those magnetic fields, getting them powerful. If you squashed the beams and focused them so that you get enough collisions, that's super. [00:23:34] Do you know how much software is involved here? I mean, it's sort of like on the software world and it's fascinating. [00:23:42] This seems like it's a software as buggy and messy. [00:23:44] And so, like, you almost don't want to rely on software too much. Like if you do, it has to be like low level, like Fortran style programming. Language software is a Large Hadron Collider. [00:23:56] I mean, it depends at which level a lot. I mean, the whole thing is obviously computer controlled. So I mean, I don't know a huge amount about how the software for the actual accelerator works. But, you know, I've been in the. Control center, so at CERN, there's this big control room, which is like a bit like NASA mission control with big banks have, you know, desks where the engineers sit and they monitor the LHC because you obviously can't be in the tunnel when it's running. [00:24:18] So everything's remote. [00:24:20] I mean, one sort of anecdote about the sort of software side in 2008 when the LHC first switched on, they had this big launch event and then, you know, big press conference party to inaugurate the machine. And about 10 days after that, they were doing some tests and the dramatic event happened where a huge explosion basically took place in the tunnel that destroyed or damaged, badly damaged about about half a kilometer of the machine. [00:24:46] But the stories the engineers are in the control room. That day, one guy told me the story about, you know, basically all these screens they have in the control room started going red. So these alarms like, you know, kind of in software going off. And then they assume that there's something wrong with the software because there's no way something this catastrophic could have could have happened. [00:25:04] Yeah, but I mean, when I worked on when I was a teacher and one of my jobs was to help to maintain the software that's used to control the detector that we work on. And that was it's relatively robust. Not so you don't want it to be too fancy. You don't want to sort of fall over to the more clever stuff comes when you're talking about analyzing the data. [00:25:25] And that's where they're sort of, you know, are we jumping around to make do we finish with a standard model? We didn't. We didn't. We started talking about quarks. We haven't talked to them yet. [00:25:34] No, we got to the masses of particles. [00:25:37] Let me go back there if it's OK. OK, that's going to take us the rest of the history of physics in the twentieth century. OK, sure. OK, so circa 1960, you have this you have these 100 or so particles. It's a bit like the periodic table all over again. So you've got like, like having 100 elements, sort of about like that and people trying to start to try to impose some order. So Murray Gellman, he's a theoretical physicist, American from New York. [00:26:04] He realizes that there are these symmetries in these particles that if you arrange them in certain ways, that they relate to each other. And he uses the symmetry principles to predict the existence of particles that haven't been discovered, which are then discovered in accelerators. So this starts to suggest there's not just random collections of crap. [00:26:21] There's like, you know, actually some order to this underlying it a little bit later in 1960, around the 1960s, he proposes, along with another physicist called George Zweig, that the symmetries arise because just like the patterns in the periodic table arise, because atoms are made of electrons and protons, that these patterns are due to the fact that these particles are made of smaller things and they are called quarks. So these are the particles that predicted from theory for a long time. [00:26:52] No one really believes that real. A lot of people think that they're a kind of theoretical convenience that happen to fit the data. But there's no evidence. No one's ever seen a quark in any experiment and lots of experiments done to try to find quarks to try to knock a quark out of a.. So the idea if protons and neutrons are made of quarks, you should wait to knock a clock out and see the quark. That never happens. And we still have never actually managed to do that. [00:27:15] We really know. [00:27:16] So the way but the way that it's done in the end is this machine that's built in California at the Stanford lab, Stanford Linear Accelerator, which is essentially a gigantic three kilometer long electron gun fires, electrons, almost speed of light at protons. [00:27:33] And when you do these experiments, what you find is a very high energy. The electrons bounce off small, hard objects inside the proton. So it's a bit like taking an X-ray of the proton. You're firing these very light high energy particles and they're pinging off. Little things inside the proton are like ball bearings, if you like. So you actually that way they resolve that there are three things inside the proton which are quarks, the quarks that Galman and Zweig had predicted. [00:28:02] So that's really the evidence that convinces people that these things are real. The fact that we've never seen one in an experiment directly, they're always stuck inside other particles. [00:28:13] And the reason for that is essentially to do with a strong force. The strong force is the force that holds quarks together and it's so strong that it's impossible to actually liberate a clock. So if you try and pull a quark out of a proton or actually ends up happening, is that the you kind of create this that this springlike bond in a strong force? Imagine two quarks that are held together by very powerful spring. You pull, pull and pull. [00:28:36] More and more energy gets stored in that bond, like stretching a spring. And eventually the tension gets so great. The spring snaps and the energy in that bond gets turned into two new quarks that go on the broken ends. So you started with two quarks. You end up with four quarks. So you never actually get to take a clock out. You just end up making loads more quarks in the process. [00:28:56] So how do we, again, forgive the dumb question. How do we know quarks are real then? [00:29:01] Well, away from these experiments where we can scatter you fire electrons into the protons. They can. Burrow into the proton and knocka and they can bounce off these quark, so you can see from the angles the electrons come out, you can infer, you can infer that these things are there. The model can also be used. [00:29:20] It has a lot of successes. So you can use it to predict the existence of new particles that hadn't been seen. So basically, there's lots of data basically showing from, you know, when we fire protons at each other at the LHC. A lot of clocks get knocked all over the place, and every time they try and escape from, say, one of their protons, they make a whole set of clocks that go flying off as bound up in other sorts of particles made of clocks. [00:29:45] So that all the sort of the theoretical predictions from the basic theory of the strong force and the clocks all agrees with what we are saying experiments. We've just never seen an actual quark on its own because unfortunately, it's impossible to get them out on their own. [00:29:58] So quarks these crazy, smaller things that are hard to imagine a real. So what else what else is part of the story here? [00:30:06] So the other thing that's going on at the time around the 60s is an attempt to understand the forces that make these particles interact with each other. So you have the electromagnetic force, which is the force that was sort of discovered to some extent in this room or at least in this building. So the first what we call quantum field theory of the electromagnetic force is developed in the 1940s and 50s by Feynman, Richard Feynman, amongst other people, Julian Suring, a Tominaga who come up with the first what we call a quantum field theory of the electromagnetic force. [00:30:42] And this is where this description of which I gave you at the beginning, that particles are ripples in fields. Well, in this theory, the photon, the particle of light is described as a ripple in this quantum field called the electromagnetic field and the attempt that is made to try what can we come up with, a quantum field theory of the other forces, of the strong force and the weak. The other the third force, which we haven't discussed, which is the weak force, which is a nuclear force. [00:31:07] We don't really experience it in our everyday lives, but it's responsible for radioactive decay is the force that allows, you know, in a radioactive atom to turn into a different element, for example. [00:31:17] And I don't know if you were explicitly mentioned, but so there's technically four forces. [00:31:22] Yes. [00:31:23] I guess three of them would be in the standard model, like the weak, the strong and the electromagnetic. [00:31:30] And then there's gravity and there's gravity, which we don't worry about that, because in this case, we bring that up at the end of the gravity. So far, we don't have a quantum theory of and if you can solve that problem, you win a Nobel Prize. [00:31:42] Well, we're going to have to bring up the graviton at some point. I'm going to ask you, but let's leave that aside for now. So those three, OK, Feynman electromagnetic force, the quantum field. Yeah. [00:31:56] So where does the weak force command. So so. [00:31:59] Yeah. Well, first of all, I mean, the strong force is the easiest, the strong force is a little bit like the electromagnetic force. It's a force that binds things together. So that's the force that holds quarks together inside the proton, for example. [00:32:09] So a quantum field theory of that force is discovered in the I think it's in the 60s and it predicts the existence of new force particles called gluons. So gluons are a bit like the photon. The photon is the particle of electromagnetism. Gluons are the particles of the strong force. So there's there's just like there's an electromagnetic field, there's something called a gluon field, which is also all around us. [00:32:36] So these are some of these particles, I guess, the force carriers or whatever, they carry them. [00:32:41] Well, it depends how you want to think about it. I mean, really, the field, the strong force field, the glue on field is the thing that binds the quarks together. [00:32:49] The gluons are the little ripples in that field so that in the same way that the photon is a ripple in the in the electromagnetic field. But the thing that really does the binding is the field. I mean, you may have heard people talk about things like virtual. You've had the phrase virtual particle. So sometimes in some if you hear people describing how forces are exchanged between particles, they quite often talk about the idea that, you know, if you have an electron and another electron say, and they're repelling each other through the electromagnetic electromagnetic force, you can think of that as if they're exchanging photons. [00:33:22] So they're kind of firing photons backwards and forwards between each other. And that causes them to repel that photons then a virtual particle. [00:33:30] Yes, that's what we call a virtual particle. In other words, it's not a real thing. It doesn't actually exist. So it's an artifact of the way theorists do calculations. So when they do calculations in quantum field theory, rather than there's no one discovered a way of just treating the whole field, you have to break the field down into simpler things so you can basically treat the field as if it's made up of lots of these virtual photons. But there's no experiment that you can do that can detect these particles being exchanged. [00:33:55] What's really happening in reality is that the electromagnetic field is warped by the charge of the electron and that causes the force. But the way we do calculations involves particles. So it's a bit confusing, but it is really a mathematical technique. [00:34:10] It's not something that corresponds to reality. [00:34:12] I mean, that's part, I guess, of the Feynman diagrams. Yes, this is virtual. That's right. Yeah. Some of these have mass. [00:34:19] Some of them don't. Is that does that or what does that even mean? Not to have mass and maybe you can say which one of them have mass, which don't. OK, so. [00:34:31] And why is mass important? All relevant in this in this in this field view of the universe. [00:34:38] Well, there are only two particles in the standard model that don't have mass, which are the photon and the gluons. So they are massless particles, but the electron, the quarks. And there are a bunch of other particles I haven't discussed. There's something called a million and a tau, which are basically heavy versions of the electron that are unstable. You can make them and accelerators, but they don't form atoms or anything. [00:35:01] They don't exist for long enough. But all the matter particles, there are 12 of them, six quarks and six what we call leptons, which includes the electron and its two heavy versions and three neutrinos. All of them have mass and so do the. This is the critical bit. So the weak force, which is the third of these quantum forces, which is one of the hardest to understand, the force particles of that force have very large masses and there are three of them. [00:35:31] They're called the W plus, the minus and the Z goes on and they have masses of between 80 and 90 times that of the the protons. They're very heavy. [00:35:42] And while they're very heavy, the what the heaviest I guess they're not the heaviest. [00:35:47] The heaviest particle is the top quark, which has a mass of about 175 ish protons. So that's really massive. [00:35:56] And we don't know why is so massive, but they're coming back to the weak force. [00:36:00] So the problem in the 60s and 70s was that the reason that the electromagnetic force is a force that we can experience in our everyday lives. [00:36:08] So if we have a magnet and a piece of metal, you can hold it, you know, a Metropol if it's powerful enough and you'll feel a force, whereas the weak force only becomes apparent when you basically have two particles touching at the scale of a nucleus. So you get to very short distances before this force becomes manifest. [00:36:26] It's not we don't get weak forces going on in this room. We don't notice them. [00:36:30] And the reason for that is that the particle, the the field that transmits the weak force, the particle that's associated with that field, has a very large mass, which means that the field dies off very quickly, says you. Whereas an electric charge, if you were to look at the shape of the electromagnetic field, it would fall off with this. You have this thing called the inverse square law, which is the idea that the force halves every time you double the distance. [00:36:55] No, sorry, it doesn't have quarters every time. Every time you double the distance between, say, the two particles, whereas the weak force kind of you move a little bit away from the nucleus and just disappears. The reason for that is because these these fields, the particles that go with them have a very large mass. [00:37:12] But the problem that was that theories faced in the 60s was that if you tried to introduce massive force fields, the theory gave you nonsensical answers. So you'd end up with infinite results for a lot of the calculations you tried to do. [00:37:28] So the basically turned out, it seemed the quantum field theory was incompatible with having massive particles, not just the force particles, actually, but even the electron was a problem. [00:37:38] So this is why the Higgs that we sort of alluded to comes in and the solution was to say, OK, well, actually all the particles in the standard model are mass. They have no mass. So the quarks, the electron, they don't have a mass. Neither do these weak particles. They don't have mass either. What happens is they actually acquire mass through another process. They get it from somewhere else. They don't actually have it intrinsically. [00:38:00] So this idea that was introduced by Peter Higgs is the most famous. But actually there are about six people that came up with the idea more or less the same time is that you introduce a new quantum field, which is another one of these invisible things that's everywhere. [00:38:14] And it's through the interaction with this field that particles get mass. So you can think of, say, an electron in the Higgs field called the Higgs field kind of bunches around the electron. It's sort of a drawn towards the electron. And that energy that's stored in that field around the electron is what we see as the mass of the electron. [00:38:36] But if you could somehow turn off the Higgs field, then all the particles in nature would become massless and fly around at the speed of light. [00:38:43] So this this idea of the Higgs field allowed other people or the theorists to come up with a well, it was another a unit, basically a unified theory of the electromagnetic force and the work force. So once you bring in the Higgs field, you can combine two of the forces into one. So it turns out the electromagnetic force and the weak force are just two aspects of the same fundamental force. [00:39:09] And at the LHC, we go to high enough energies that you see these two forces unifying effectively. [00:39:16] So so first of all, it started as a theoretical notion like this. [00:39:22] And then it wasn't the Higgs called the God particle. At some point it was by a guy trying to sell popular science books. [00:39:30] Yeah, yeah. But. I mean, I remember when I was hearing it, I thought it would. I mean, that would solve a lot of the unify a lot of our ideas of physics was my notion, but maybe you can speak to that was as big of a leap. [00:39:47] Is that as a God particle, that Jesus particle at which which, you know, what's the big contribution of Higgs in terms of this unification power? [00:39:57] Yeah, I mean, to understand that it maybe helps know the history a little bit. So when the what we call electroweak theory was put together, which is where you unify electromagnetism with a weak force and the Higgs is involved in all of that. So that theory, which was written in the mid 70s, predicted the existence of four new particles. The plus both on the minus goes on, the Z Bo's on, and the Higgs boson. So there were these four particles that came with the theory that were predicted by the theory in 1983, 84, the W's and the Z particles were discovered an accelerator at CERN called the Super Proton Synchrotron, which was a seven kilometer particle collider. [00:40:36] So three of the bits of this theory had already been found. So people were pretty confident from the 80s that the Higgs must exist because it was a part of this family of particles that this theoretical structure only works if the Higgs is there. So what then happens? So this question of why is the LHC the size it is? Yes. Well, actually, the tunnel that the LHC is in was not built for the LHC. It was built from for a previous accelerator called the Large Electron Positron Collider. [00:41:05] So that that was began operation in the late 80s, early 90s. [00:41:10] They basically that's when they dug the 27 kilometer tunnel. They put this accelerator into a collider that fires electrons and anti electrons at each other, electrons and positrons. [00:41:19] So the purpose of that machine was, well, it was actually to look for the Higgs. That was one of the things it was trying to do. It didn't matter. It didn't have enough energy to do it in the end. [00:41:28] But the main thing it achieved was it studied the W and the Z particles at very high precision. So it made loads of these things previously, only make a few of them at the previous accelerator. So you could study these. Really, really, precisely. And by studying their properties, you could really test this electroweak theory that had been invented in the 70s and really make sure that it worked. So actually by 1999, when this machine turned off, people knew. [00:41:54] Well, you never know until you until you find the thing. But people were really confident this electroweak theory was right and that the Higgs, almost the Higgs or something very like the Higgs had to exist because otherwise the whole thing doesn't work. It'd be really weird if you could discover and these particles, they all behave exactly as a theory, tells you they should. But somehow this key piece of the picture is not there. [00:42:17] So in a way, it depends how you look at it. [00:42:20] The discovery of the Higgs on its own is is a huge achievement in many, both experimentally and theoretically. On the other hand, it's this it's like having a jigsaw puzzle where every piece has been filled in this beautiful image. [00:42:34] There's one gap and you kind of know that that piece must be there somewhere. Right? [00:42:39] So if so, the discovery in itself, although it's important. Is not so interesting. It's a confirmation of the obvious at that point. But what makes it interesting is not it just completes the standard model, which is a theory that we've known had the basic layout office for 40 years or more. Now it's that the Higgs actually is a is a unique particle, is very different to any of the other particles in the standard model. And it's a theoretically very troublesome particle. [00:43:12] There are a lot of nasty things to do with the Higgs, but also opportunities. [00:43:17] So we basically don't really understand how such an object can exist in the form that it does. So there are lots of reasons for thinking that the Higgs must come with a bunch of other particles or that it's perhaps made of other things. So it's not a fundamental particle that it's made of smaller things. I can talk about that, if you like a bit. [00:43:36] That's still a notion. So, yeah. So so the Higgs might not be a fundamental particle that there might be some in my old man. [00:43:44] So that that is an idea is not you know, there's not been demonstrated to be true. But I mean, there's all of these ideas basically come from the fact that. [00:43:53] Is this is this is a problem that motivated a lot of development in physics in the last 30 years or so, and there's this basic fact that the Higgs field, which is this field that's everywhere in the universe, this is the thing that gives mass to the particles and the Higgs field is different from all the other fields in that, let's say you take the electromagnetic field, which is, you know, if we actually have to measure the electromagnetic field in this room, we would measure all kinds of stuff going on because there's light, there's going to be microwaves and radio waves and stuff. [00:44:19] But let's say we go to really, really remote part of empty space and shield it and put a big box around it and then measure the electromagnetic field in that box. The field would be almost zero apart from some little quantum fluctuations, but basically it goes to naught. The Higgs field has a value everywhere. So it's a bit like the whole like the entire of space has got this energy stored in the Higgs field, which is not zero. [00:44:42] It's it's finite. It's got some it's a bit like having the the temperature of space raised to, you know, some background temperature. And it's that energy that gives mass to the particles. So the reason that electrons and quarks have mass is through the interaction with this energy that's stored in the Higgs field. [00:45:01] Now, it turns out that the precise value of this energy has has to be very carefully tuned if you want a universe where interesting stuff can happen. So if you push the Higgs field down, it has a tendency to collapse to what? There's a tent. If you do your sort of naïf calculations, there are basically two possible likely configurations for the Higgs field, which is either it's zero everywhere, in which case you have a universe, which is just particles with no mass that can't form atoms and just fly about the speed of light or it explodes to an enormous value, what we call the Planck scale, which is the scale of quantum gravity. [00:45:41] And at that point, if the Higgs field was that strong, even an electron would become so massive that it would collapse into a black hole. And then you have a universe made of black holes and nothing like us. [00:45:51] So it seems that the strength of the Higgs field is to actually achieve the value that we see requires what we call fine tuning of the laws of physics. You have to fiddle around with the other fields in the standard model and their properties to just get it to this right sort of Goldilocks value that allows atoms to exist. [00:46:10] This is deeply fishy. People really dislike this. [00:46:14] Well, yeah, I guess so. What would be two explanations? One, there's a God, the design this perfectly. And two is there's an infinite number of alternate universes and we just happen to be in the one in which life is possible. Yeah, complexity. So when you say I mean life, any kind of complexity, that's not either complete chaos or black holes. Yeah, yeah. I mean, how does that make you feel? [00:46:39] What do you make that such a fascinating notion that this perfectly tuned field. That's the same everywhere. Yeah. Is there. What do you make of that. Yeah. [00:46:50] What do you make of that. I mean, yes, you laid out two of the possible explanations. Yeah. I mean, someone you know, some cosmic creator. Well, yeah. Let's fix that. Be at the right level. That's one possibility. I guess it's not a scientifically testable one. But, you know, theoretically, I guess it's possible. [00:47:05] Sorry to interrupt, but there could also be not a designer. But couldn't there be just I guess I'm not sure what that would be, but some kind of force that. That some kind of mechanism by which this this. This kind of field is enforced in order to create complexity, basic basically forces that. Paul, the universe towards an interesting complexity, I mean, yeah, I mean, those ideas, I don't really subscribe to them. [00:47:40] As I'm saying, it sounds really stupid. No, I mean, there are definitely people that make those kind of arguments, you know, those ideas that I think it's least Merlin's idea. I think that, you know, universes are born inside black holes. [00:47:55] And so universe is the have of Darwinian evolution of the universe where universes give birth to other universes. And if universes where black holes can form are more likely to give birth to more universes. So you end up with universes which have similar laws. I mean, I don't know whatever. [00:48:09] But I talked to Dr. Lee recently on this podcast, and he's he's a reminder to me that the physics community has like so many interesting characters. Yeah, it's fascinating. Anyway, so so, I mean, as an experimentalist, I tend to sort of think these are interesting ideas, but they're not really testable. So I tend to think about it very much. So. I mean, going back to the science of this, there wasn't there is an explanation. [00:48:36] There is a possible solution to this problem of the Higgs, which doesn't involve multiverses or creators fiddling about with the laws of physics. If the most popular solution was something called supersymmetry, which is a theory which is inveigle involves a new type of symmetry of the universe. In fact, it's one of the last types of symmetries that is possible to have that we haven't already seen in nature, which is a symmetry between force particles and matter particles. [00:49:01] So what we call fermions, which are the matter particles and bosons, which are force particles. [00:49:06] And if you have supersymmetry, then there is a super partner for every particle in the standard model and the without going into details, the effect of this basically is that you have a whole bunch of other fields and these fields cancel out the effect of the standard model fields and they stabilize the Higgs field at a nice, sensible value. So in supersymmetry, you naturally, without any tinkering about with the constants of nature or anything, you get Higgs field with a nice value, which is what we see. [00:49:35] So this is one of the supersymmetry is also got lots of other things going for it. It predicts the existence of a dark matter particle, which would be great. You know, it potentially suggests that the strong force and the electroweak force unify energy. So lots of reasons. People thought this was a productive idea. And when the LHC was just before it was turned on, there was a lot of hype, I guess a lot of an expectation that we would discover these super partners because and particularly the main reason was that if if supersymmetry stabilises the Higgs field at this nice Goldilocks value, these super particles should have a mass around the energy that we're probing at the LHC around the energy of the Higgs. [00:50:16] So it was kind of thought you discovered the Higgs. You probably discover super partners. So once you start creating ripples in this Higgs field, you should be able to see these kinds of it should be super fields would be there. [00:50:27] And at the very beginning, I said we're probing the vacuum. What I mean is really that, you know, let's say these super fields exist. The vacuum contains super fields. There were these supersymmetric fields. If we hit them hard enough, we can make them vibrate. We see super particles come flying out. That's the sort of that's the idea. [00:50:43] That's the whole point. But we haven't. But we haven't. So so far at least, I mean, we've had now a decade of data taking at the LHC. No signs of super partners have supersymmetric particles have been found. In fact, no signs of any physics, any new particles beyond the standard model have been found. So supersymmetry is not the only thing that can do this. There are other theories that involve additional dimensions of space or potentially involve the Higgs boson being made of smaller things being made of other particles. [00:51:15] Yeah, that's an interesting you know, I haven't heard that before. That's really that's an interesting point, because you maybe linger on that. Like what what could be what could the Higgs particle be made of? [00:51:25] Well, so the oldest I think the original ideas about this was these theories called Technicolor, which were basically like an analogy with the strong force. [00:51:34] So the idea was the Higgs boson was a bound state of two very strongly interacting particles that were a bit like quarks. So like quarks, but I guess higher energy things with a super strong force and not the strong force, but a new force that was very strong. And the Higgs was a bound state of of these these objects and the Higgs boson principle, if that was right, would be the first in a series of Technicolor particles, Technicolor, I think not being a theorist, but is not based basically not done very well, particularly since the LHC found the Higgs. [00:52:06] That kind of it rules out, you know, a lot of these Technicolor theories. But there are other things that are a bit like Technicolor. So there's a theory called partial composite ness, which is an idea that some of my colleagues at Cambridge have worked on, which is a similar sort of idea that the Higgs is a bound state of some strongly interacting particles and that the standard model particles themselves, the more exotic ones like the top. They are also sort of mixtures of these composite particles, so it's a kind of an extension to the standard model which explains this problem with the Higgs boson is Goldilocks value, but also helps us understand we have we're in this situation now, again, a bit like the periodic table where we have six quarks, six leptons in this kind of range, in this nice table. [00:52:56] And there you can see these columns where the patterns repeat and you go, OK, maybe there's something deeper going on here, you know? And so this would potentially be something this partial composite theory could explain a sort of enlarge this picture that allows us to see the whole symmetrical pattern and understand what the ingredients. Why do we have. So one of the big questions in particle physics is why are there three copies of the matter particles? [00:53:23] So in what we call the first generation, which is what we're made of, there's the electron, the electron neutrino, the up quark and the down quark. They're the most common matter particles in the universe. But then there are copies of these four particles in the second and third generations. So things like muons and top quarks and other stuff, we don't know why we see these patterns. We have no idea where it comes from. So that's another big question. [00:53:45] You know, can we find out the deeper order that explains this particular type periodic table of particles that we see is the possible that the the deeper order includes like almost a single entity. [00:53:59] So like something that I guess like string theory dreams about is this is this is this is this essentially the dream is to discover something simple, beautiful, unifying. [00:54:10] Yeah. I mean, that is the dream. And or I think for some people, for a lot of people it still is the dream. [00:54:17] So there's a great book by Steven Weinberg, who is one of the theoretical physicists who was instrumental in building the standard model. So he came up with some others with the electroweak theory, the theory that unified electromagnetism and the weak force. And he wrote this book, I think it was towards the end of the 80s, early 90s, called Dreams of a Final Theory, which is a very lovely, quite short book about this idea of a final unifying theory that brings everything together. [00:54:44] And I think you get a sense, reading his book written at the end of the 80s, early 90s, that there was this feeling that such a theory was coming. And that was the time when string theory had been was was very exciting. So string theory, there's been this thing called the super string revolution and theoretical physics are very excited. They discovered these theoretical objects, these little vibrating loops of string that in principle not only was a quantum theory of gravity, but could explain all the particles in the standard model and bring it all together. [00:55:12] And as you say, you have one object, the string, and you can pluck it. And the way it vibrates gives you these different notes, each of which is a different particle. So it's a very lovely idea. [00:55:25] But the problem is that there's there's a few people discovered the mathematics is very difficult. So people have spent three decades more trying to understand string theory. And I think, you know, if you spoke to my string theorists, they would probably freely admit that no one really knows what string theory is yet. I mean, there's been a lot of work, but it's not really understood. [00:55:44] And the other problem is that string theory mostly makes predictions about physics that occurs at energies far beyond what we will ever be able to probe in the laboratory. Yeah, probably ever, by the way, to say take a million tangents. [00:56:01] But is there room for complete innovation of how to build a particle collider that could give us an order of magnitude increase? And in the kind of energies or do we need to keep just increasing the size of the thing? [00:56:15] I mean, maybe yeah. I mean, there are ideas to give you a sense of the Gulf that has to be bridged. So the LHC collides particles at an energy of what we call 14 terra electron volts. So that's basically equivalent of you accelerated a proton through 14 trillion volts. That gets us to the energies where the Higgs and these weak particles live. They're very massive. The scale where strings become manifest is something called the Planck scale, which I think is of the order. [00:56:47] Ten to the hang on. It's right is ten to eighteen giga electron volts. So about 10 to the 15 Tera electron volts. So you're talking, you know, trillions of times more energy, more than 10 to the 15 attended the 14th larger. [00:57:06] I think it's a very big number. So, you know, we're not talking just an order of magnitude increase in energy. We're talking 14 orders of magnitude energy increase. So to give you a sense of what that would look like, were you to build a particle accelerator with today's technology bigger or smaller than our solar system, a site the size of the galaxy, the galaxy. [00:57:27] So you need to put a particle accelerator that circled the Milky Way to get. The energy is where you would see strings if they exist, so that is a fundamental problem, which is that most of the predictions of the unified, this unified theory, quantum theory of gravity only make statements that are testable at energies that we will not be able to probe. [00:57:49] And barring some unbelievable, you know, completely unexpected technological or scientific breakthrough, which is almost impossible to imagine, you never, never say never, but it seems very unlikely. [00:57:59] Yeah, I can just see the news story. Elon Musk decides to build a particle collider the size of our. [00:58:07] It would have to be we'd have to get together with all our galactic neighbors to to pay for it. [00:58:11] I think what is the exciting possibilities is the Large Hadron Collider. What is there to be discovered in this in this order of magnitude of scale? [00:58:21] Is there other bigger efforts on the horizon in this space where the open problems, the exciting possibilities? You mentioned supersymmetry. Yeah. [00:58:32] So well, there are lots of new ideas. Well, there are lots of problems that we're facing. So there's a problem with the Higgs field, which supersymmetry was supposed to solve. There's the fact that 95 percent of the universe we know from cosmology, astrophysics is invisible, that it's made of dark matter and dark energy, which are really just words for things that we don't know what they are. That's what Donald Rumsfeld called a known unknown. We know we don't know what they are. [00:58:56] Well, that's better than unknown unknown unknowns. Yeah, well, there may be some unknown unknowns, but we don't know what those are. [00:59:03] So, yeah, but the hope is the particle accelerator could help us make sense of dark energy, dark matter. There's still there's some hope for that. There's hope for that. [00:59:15] Yes. So one of the hopes is the LHC could produce a dark matter particle in its collisions. [00:59:20] And, you know, it may be that the LHC will still discover new particles, that it might still supersymmetry could still be there. We just it's just maybe more difficult to to find than we thought originally. And, you know, dark matter particles might be being produced, but we're just not looking in the right part of the data for them that that's possible. It might be that we need more data, that these processes are very rare and we need to collect lots and lots of data before we see them. [00:59:44] But I think a lot of people would say now that the chances of the LHC directly discovering new particles in the near future is quite slim. It may be that we need a decade more data before we can see something or we may not see anything. That's the that's why we are so I mean, the physics, the experiments that I work on. So I work on a detector called LHC B, which is one of these four big detectors that are spaced around the ring. [01:00:11] And we do slightly different stuff to the big guys. There's two big experiments, Cloud Atlas and CMS. Three thousand physicists and scientists and computer scientists on them each day are the ones that discovered the Higgs and they look for supersymmetry and dark matter and so on. [01:00:25] While we look at our standard model particles called B quarks, which depending on your preferences, either bottom or beauty, we tend to say beauty because it sounds sexier. [01:00:35] Yeah, for sure. [01:00:37] But these particles are interesting because they of we can make lots of them. We make billions and billions, hundreds of billions of these things. You can therefore measure their properties very precisely so you can make these really lovely precision measurements. [01:00:51] And what we are doing really is a sort of complementary thing to the other big experiments, which is they if you think of analogy, they often use is imagine you're looking in you're in a jungle and you're looking for an elephant, say, and you are a hunter and you're kind of like that said as the relevance, very rare. [01:01:10] You don't know where in the jungle the jungles, because there's two ways you go about this. Either you can go wandering around the jungle and try and find the elephant. The problem is, if the elephant is there's only one elephant in the jungle, bigger chances of running into a very small or you could look on the ground and see if you see footprints left by the elephant. And if the elephants moving around, you've got a chance that a chance maybe of seeing the elephants footprints. [01:01:30] If you see the footprints, you go, OK, there's an elephant. Maybe don't know what kind of elephant it is, but I got a sense there's something out there. So that's sort of what we do. We are the footprint people. [01:01:40] We we are we're looking for the footprints, the impressions that quantum fields that we haven't managed to directly create the particle of the effects these quantum fields have on the ordinary standard model fields that we already know about. So these these big particles, the way they behave, can be influenced by the presence of, say, super fields or dark matter fields or whatever you like. And the way they decay and behave can be altered slightly. From what our theory tells us, they ought to behave. [01:02:09] And it's easier to collect huge amounts of data and be unbe quarks. We get, you know, billions and billions of these things. You can make very precise measurements. And the only place really at the LHC or really in high energy physics at the moment, where there's a fairly compelling evidence that there might be something beyond the standard model is in these B. These beauty kwok's the case, just to clarify, which is the difference between the different the four experiments, for example, that you mentioned, is that the kind of particles that are being collided is that the energies of which they're collided? [01:02:44] What was the fundamental difference is the different experiments, the collisions of the same. [01:02:49] What's different is the design of the detectors. So Atlas and CMS are called they're called what are called general-purpose detectors, and they are basically barrel shaped machines. And the collisions happen in the middle of the barrel and the barrel captures all the particles that go flying out in every direction. So in a sphere, effectively, they come flying out and it can record all of those particles. [01:03:08] And what's the. So to be interrupting. But what's what's the mechanism of the recording? [01:03:14] Oh, these detectors, if you're seeing pictures of the huge like Atlas is 25 metres high in forty metres long and vast machines, instruments, I guess you could call them really. [01:03:26] They are they're kind of like onions. [01:03:28] So they have layers, concentric layers of detector detectors, different sorts detectors. So close into the beam pipe you have what are called usually made of silicon. They're tracking detectors. So they're little made of strips of silicon or pixels of silicon. And when a particle goes through the silicon, it gives a little electrical signal and you get these dots, you know, electrical dots through your detector, which allows you to reconstruct the trajectory of the particle. So that's the middle. [01:03:51] And then the outside of these detectors, you have things called calorimeter, which measure the energies of the particles and the very edge. You have things called muon chambers, which basically these Muan particles, which are the heavy version of the electron, they are they like high velocity bullets and they can get right to the edge of the detectors if you see something at the edge that's immune. [01:04:09] So that's broadly how they work. And all of that is being recorded. That's all being fed out to computers. [01:04:15] Data must be awesome. OK, so LHC is different. So we because we're looking for these B quarks. Yes. B quarks tend to be produced along the beamlines. So in a collision, the B tend to fly sort of close to the beam pipe. So we built the detector, that sort of pyramid cone shaped basically that just looks in one direction. So we ignore, give you a collision, stuff goes everywhere. We ignore all the stuff over here and going off sideways. [01:04:40] We're just looking in this little region close to the beam pipe where most of these big quarks are made. [01:04:45] So is there a different aspect of the sensors involved in the collection of the big quark? Is there are some differences. So one of the differences is that one of the ways, you know, you've seen a big walk is that B, corks are actually quite long lived by particle standards. So they live for one point five trillionths of a second, which is if you if you're a fundamental particle is a very long time. Because, you know, the Higgs boson, I think, lives for about a trillionth of a trillionth of a second or maybe even less than that. [01:05:15] So these are quite long lived things and they will actually fly a little distance before they decay. So they will fly, you know, a few centimetres. Maybe if you're lucky, then they'll decay into other stuff. So what we need to do in the middle of the detector, you want to be able to see you have your place where the protons crash into each other and that produces loads of particles that come flying out. So you have loads of lines, loads of tracks that point back to that proton collision. [01:05:38] And then you're looking for a couple of other tracks, maybe two or three, that point back to a different place that maybe a few centimetres away from the proton collision. And that's the sign that little B particle has flown a few centimetres and decayed somewhere else. [01:05:50] So we need to be able to very accurately resolve the proton collision from the B particle decay. [01:05:56] So we are the middle of our detector is very sensitive and it gets very close to the collisions. So you have this really beautiful, delicate silicone detector that sits I think it's seven mil millimeters from the beam. And the LHC beam has as much energy as a jumbo jet take off. So it's enough to melt a ton of copper. So you have this furiously powerful thing sitting next, this tiny, delicate silicon sensor. [01:06:20] So those aspects of architecture that are specialized to to to measure these particular B quarks that we're interested in. [01:06:27] And is there I mean, I remember seeing somewhere that there is some mention of matter and antimatter connected to the B, the these beautiful quarks. Is that what's the connection? Yeah. What's the connection there? [01:06:42] Yes, there is a connection, which is that when you produce these big particles, these particles actually to be quark, you see the thing that be quark is inside. [01:06:52] So they're bound up inside what we call beauty particles, where the big quokkas joined together with another quark or two, maybe two other quarks, depending on what it is. They're a particular set of these big particles that exhibit this property called oscillation. So if you make a for the sake of argument, amateur version of one of these B particles as it travels because of the magic of quantum mechanics, it oscillates backwards and forwards between its matter and antimatter versions. [01:07:20] So does this weird flipping about backwards and forwards. And what we can use this for is a laboratory for testing the symmetry between matter and antimatter. So if the if the symmetry between our two countries is precise, it's exact, then we should see these big particles decaying as often as matters. That doesn't matter, because this oscillation should be even it should spend as much time in each state. But what we actually see is that one of the states spends more time and it's more likely to decay in one state than the other. [01:07:49] So this gives us a way of testing this fundamental symmetry between matter and antimatter. [01:07:56] So what can you sort of return to the question before about this fundamental symmetry? It seems like if there's perfect symmetry between matter and antimatter, if we have the equal amount of each in our universe, it would just destroy itself. And just like you mentioned, we seem to live in a very unlikely universe where it doesn't destroy itself. Yeah. So just some intuition about why that is. [01:08:24] I mean, well, I'm not a theory. I don't have any particular ideas myself. I mean, I sort of do measurements to try and test these things. But I mean, the terms of the basic problem is that in the Big Bang, if you use the standard model to figure out what ought to have happened, you should have got equal amounts of matter and antimatter made. Because whenever you make a particle in our collisions, for example, when we collide stuff together, you make a particle, you make an antiparticle, they always come together, they always annihilate together. [01:08:47] So there's no way of making more matter and antimatter that we've discovered so far. So that means in the big bang, you get equal amounts of matter and antimatter as the universe expands and cools down during the Big Bang not very long after the Big Bang. [01:09:00] I think a few seconds after the Big Bang, you have this event called the Great Annihilation, which is where all the particles and antiparticles smack into each other annihilate, turn into light mostly, and you end up with a universe later. Or if that was what happened in the universe we live in today would be black and empty. Apart from some photons, that would be it. So there's stuff in this. There is stuff in the universe. It appears to be just made of matter. [01:09:22] There's this big mystery as to where the how did this happen? And there are various ideas. Which all involve sort of physics going on in the first trillionth of a second or so of the Big Bang, so it could be that one possibility is that the Higgs field is somehow implicated in this, that there was this event that took place in the early universe where the Higgs field basically switched on. It acquired its modern value. [01:09:48] And when that happened, this caused all the particles to acquire mass. And the universe basically went through a phase transition where you had a hot plasma of massless particles. And then in that plasma, it's almost like a gas turning into droplets of water. You get kind of these little bubbles forming in the universe where the Higgs field has acquired its modern value. Particles have got mass and this phase transition in some models can cause more matter and antimatter to be produced depending on how matter bounces off these bubbles in the early universe. [01:10:18] So that's one idea. There's other ideas to do with neutrinos, that there are exotic types of neutrinos that can decay in a biased way to just matter and not to actually matter. So people are trying to test these ideas. That's what we're trying to do at LHC base. There's neutrino experiments planned. They're trying to do these sorts of things as well. So, yeah, there are ideas, but at the moment, no clear evidence for which of these ideas might be right. [01:10:39] So we're talking about some incredible ideas, by the way, never heard anyone be so eloquent about describing even just the standard model. So, I mean, I just think interesting. [01:10:52] Just having fun, enjoying it. So the yes, the theoretical the particle physics is fascinating here. To me, one of the most fascinating things about the Large Hadron Collider is the human side of it that a bunch of. Sort of brilliant people that probably have egos got together and will collaborate together and countries, I guess collaborate together, you know, for the funds and everything, just collaboration everywhere, because you maybe I don't know what the right question here to ask almost was your intuition about how is it possible to make this happen and what are the lessons we should learn for the future of human civilization in terms of our scientific progress? [01:11:34] Because it seems like this is a great, great illustration of us working together to do something big. [01:11:41] Yeah, I think it's possibly the best example maybe I can think of of international collaboration that isn't for some unpleasant purpose. Basically, you know, is I mean, so I when I started out in the field in 2008 as a new student, the LHC was basically finished. So I didn't have to go around asking for money for it or trying to make the case. So I have huge admiration, admiration for the people who managed that, because this was a project that was first imagined in the 1970s. [01:12:09] In the late 70s was when the first conversations about the LHC were mooted. [01:12:13] And it took two and a half decades of campaigning and fundraising and persuasion until they started breaking ground and building the thing in the early noughties in 2000. [01:12:24] So, I mean, I think the reason just from a sort of from the point of view of the sort of science the scientists there, I think the reason it works ultimately is that everywhere, everyone there is there for the same reason, which is, well, in principle, at least they're there because they're interested in the world. They want to find out, you know, what are the basic ingredients of our universe, what are the laws of nature. [01:12:47] And so everyone is pulling in the same direction. Of course, everyone has their own things they're interested in. Everyone has their own careers to consider. And, you know, I wouldn't pretend that there isn't also a lot of competition. So there's this funny thing in these experiments where your collaborators, your eight hundred collaborators in LHC, but you're also competitors because your academics and your various universities and you want to be the one that gets the paper out on the most exciting new measurement. [01:13:10] So there's this funny thing where you're kind of trying to stake out your territory while also collaborating and having to work together to make the experiments work. And it does work amazingly well actually, considering all of that. [01:13:22] And I think there was actually I think McKinsey or one of these big management consultancy firms went into CERN maybe a decade or so ago to try to understand how these organizations functioned. [01:13:32] They figure it out that they think they could. I mean, I think one of the things that interesting, one of the other interesting things about these experiments is that they're big operations like, say, Atlas. Three thousand people. [01:13:41] Now, there was a person nominally who is the head of Atlas. They're called the spokesperson. And the spokesperson is elected by usually by the collaboration. [01:13:51] But they have no actual power, really. I mean, they can't fire anyone. They're not anyone's boss. [01:13:56] So, you know, my boss is is a professor at Cambridge, not the head of my experiments. The head of my experiment can't tell me what to do, really. And that's all you've got is independent academics who are their own bosses, who, you know, so somehow it nonetheless, by kind of consensus and discussion and lots of meetings, these things do happen and it does get done. [01:14:18] But it's like the queen here in the UK is the spokesperson against those who actually say we don't elect her. [01:14:23] No, go after whatever everybody seems to love or don't know from the outside perspective. [01:14:33] But, yeah, giant egos, brilliant people, and moving forward, do you think there's actually I would pick up one thing you said just that just the brilliant people thing, because I'm not I'm not saying that people aren't great, but I think there is this sort of impression that physicists will have to be brilliant or geniuses, which is not true, actually. And, you know, you have to be relatively bright for sure. [01:14:54] But, you know, a lot of people, a lot of the most successful experimental physicists are not necessarily the people with the biggest brains that the people who, you know, particularly one of the skills that are most important in particle physics is the ability to work with others and to collaborate and exchange ideas and also to work hard. And it's the sort of often it's more determination or a sort of other set of skills is not just being, you know, kind of some great brain virtuoso. [01:15:19] I mean, there's parallels to that in the machine learning world. If you want to if you want to solve any real world problems, which I see as the the particle accelerator is essentially a real world instantiation of theoretical physics. And for that, you have to not necessarily be brilliant, but be sort of obsessed, systematic, rigorous, sort of unbearable Stober and all those kind of qualities that make for a great engineer. So the science scientist, purely speaking, that practitioner of the scientific method say you're right. [01:15:54] But nevertheless, to me, that's to me as my dad, as a physicist, I argue with him all the time. To me, engineering is the highest form of science and he thinks that's all nonsense, that the real work is done by the theoreticians. So in fact, we have arguments about like people like Elon Musk, for example, because I think his work is quite brilliant. But he's fundamentally not coming up with any serious breakthroughs. He's just creating in this world, implementing. [01:16:23] I like making ideas happen to have a huge impact to me. That is that's the Edison. That to me is is a brilliant work. But to him, it's you know, it's messy details that somebody will figure out anyway. [01:16:42] I mean, I don't know whether you think there is an actual difference in temperament between, say, a physicist and an engineer, whether it's just what you got interested in, I don't know. [01:16:51] I mean, a lot of what experimental physicists do is, to some extent, engineering. I mean, it's not why do I mostly do data stuff? But, you know, a lot of people would be called electrical engineers, but they trained as physicists, but they learn electrical engineering, for example, because they were building detectors. So there's not such a clear divide, I think. [01:17:09] Yeah, it's interesting. I mean, there does seem to be like you work with data, does seem to be a certain like I love data collection. [01:17:18] There may be an OCD element or something that you're more naturally predisposed to as opposed to like I'm not afraid of data. I love data. [01:17:27] And there's a lot of people machine learning or more like they're basically afraid of data collection, afraid of data sets, afraid of all that. They just want to stay in more than theoretical and they're really good at it. Space. I don't know if that's genetic. That's your upbringing, the way you were, the way you go to school, but looking into the future of LHC and other colliders. [01:17:50] So there's in there in America, there is, whatever it was called, a super there's a lot of superconducting supercollider supercollider in the desert from Desert Itron. Yeah. So that was cancelled. The construction of that, you know, of, which is a sad thing. But what do you think is the future of these efforts with a bigger collider to be built will be expanded. What do you think? [01:18:16] Well, in the near future, the LHC is going to get an upgrade. So that's pretty much confirmed. I think it is confirmed, which is it's not an energy upgrade. It's what we call a luminosity upgrade. So basically means increasing the data collection rates. [01:18:30] So more collisions per second, basically because after a few years of data taken, you get this law of diminishing returns where each year's worth of data is a smaller and smaller fraction of the lot. You've only got to to get a real improvement in sensitivity. You need to increase the data rate by an order of magnitude. So that's what this upgrade is going to do. LHC be the moment the whole detector is basically being rebuilt to allow it to record data at a much larger rate than we could before. [01:18:54] So that will make us sensitive to whole loads of new processes that we weren't able to study before. And, you know, I mentioned briefly these anomalies, anomalies that we've seen. [01:19:02] So we've seen a bunch of very intriguing anomalies in these B quark decays, which may be hinting at the first signs of this kind of the elephant, you know, the signs of some new quantum field or fields maybe beyond the standard model. It's not yet at the statistical threshold where you can say that you've observed something, but there's lots of anomalies in many measurements that all seem to be consistent with each other. So it's quite interesting. So, you know, the upgradable allow us to really have. [01:19:31] I mean, on these things and see whether these challenges are real, because if they are real and this kind of connects to your point about the next generation of machines, what we would have seen then is, you know, we will have seen the tail end of some quantum field in influencing these big cork's. What we then need to do is to build a bigger collider to actually make the the particle of that field. So if these if these things really do exist. [01:19:57] So that would be one argument. I mean I mean, so at the moment, Europe is going through this process of thinking about the strategy for the future. So there are a number of different proposals on the table. One is for a sort of higher energy upgrade of the LHC where you just build more powerful magnets and put them in the same tunnel. That's a sort of cheap, cheaper, less ambitious possibility. Most people don't really like it because it's sort of a bit of a dead end, because once you've done that, there's nowhere to go. [01:20:22] There's a machine called Kallick, which is a compact, linear collider, which is an electron positron collider that uses a novel type of acceleration technology to accelerate shorter distances. We're still talking kilometres long, but not like 100 kilometres long. And then the probably the project that is, I think, getting the most support. They'll be interested to see what happens. Something called the Future Circular Collider, which is a really ambitious long term multi decade project to build a 100 km circumference tunnel under the Geneva region. [01:20:55] The LHC would become a kind of feeding machine. [01:20:57] It would just feed for the same area. So there would be a theater for the. Yeah. So it would kind of the machine would be where the LHC is, but it would sort of go under Lake Geneva and round the Alps basically, you know, up to the edge of the Geneva Basin. So its base, the biggest it's the biggest tunnel you can fit in the region based on the geology kilometres. Yes, it's big. It'd be a long drive. [01:21:16] If you're experiments on one side, you've got to go back to CERN for lunch. So that would be a pain for. [01:21:22] But, you know, so this project is in principle is actually to accelerate as the first thing you would do is put an electron positron machine in the 100 km tunnel to study the Higgs. You'd make lots of Higgs boson study it really precisely in the hope that you see it misbehaving and doing something that's not supposed to. And then in the much longer term, one that gets taken out, you put in a proton proton machine. So it's like the LHC, but much bigger and bigger. [01:21:45] And that's the way you start going and looking for dark matter or you're trying to recreate this phase transition. I talked about in the early universe where you can see matter and antimatter being made, for example, there are lots of things you can do with these machines. [01:21:58] The problem is that they will take, you know, the most optimistic. You're not going to have any data from any of these machines until 2040 or, you know, because they take such a long time to build and they're so expensive. So you have a process of R&D design and also the political case being made. [01:22:14] So LASU cost a few billion. Depends how you count it. I think most of the sort of more reasonable estimates that take everything into account properly. It's around the sort of 10, 11, 12 billion euro mark. [01:22:27] What would be the future? So I forgot the future circular collider for Future Circular. Presumably they won't call it that when it's built because it won't be the future anymore, but they'll call it that. The very Big Hadron Collider, I don't know. But that will I know I should know the numbers, but I think the whole project is estimated at about 30 billion euros. But that's money spent over between now and 2017, probably, which is when the last bit of it would be sort of finishing up, I guess. [01:22:59] So you're talking a half a century of science coming out of this thing shared by many countries. So the actual cost, the arguments that are made is that you could make this project fit within the existing budget of CERN if you didn't do anything else. [01:23:14] CERN, by the way, we didn't mention what is CERN? [01:23:17] CERN is the European Organization for Nuclear Research. It's an international organization that was established in the 1950s in the wake of the Second World War as a kind of it was sort of like a scientific Marshall Plan for Europe. The idea was that you bring European science back together for peaceful purposes, because what happened in the forties was, you know, a lot of particular jury scientists, but a lot of scientists from Central Europe had fled to the United States and Europe had sort of seen this brain drain. [01:23:44] So as a desire to bring the community back together for a project that wasn't building nasty bombs but was doing something that was curiosity driven. So and that has continued since then. So it's kind of a unique organisation. It's you to be a member as a country. You sort of sign up as a member and then you have to pay a fraction of your GDP each year as a subscription. I mean, it's a very small fraction, relatively speaking. [01:24:06] I think it's like I think the UK's contribution is 100 or 200 million quid or something like that. Yeah. [01:24:12] Which is quite a lot, but not that fast. I mean, just the whole thing that is possible. It's beautiful. It's a beautiful idea, especially with when there's no wars on the line. Is that like we're freaking out as we actually legitimately collaborating to do good science? One of the things I don't think we really mention is on the final side that sort of the data. Nelson said, is a breakthrough is possible there and the machine learning is there. [01:24:36] Is there a lot more signal to be mined in more effective ways from the actual raw data? Yeah, a lot of people are looking into that. [01:24:44] I mean, know I'll use machine learning in my data analysis, but pretty nodi, you know, basic stuff because I'm not a machine learning expert. I'm just a physicist who had to learn to do this stuff from my day job. So while a lot of people do is they use kind of off the shelf packages that you can train to do signal noise, you know, just clean up or. [01:25:04] Yeah, but one of the big challenges, you know, the big challenge of the data is a it's volume. There's huge amounts of data. So the LHC generates now about the actual numbers are. But if we don't record all our data, we record a tiny fraction of the data. It's like Avoda one 10000 or something. I think that right around that. So it's mostly it's thrown away. You couldn't record or the LHC data because it would fill up every computer in the world in a matter of days, basically. [01:25:30] So there's this process that happens on live on the detector, something called a trigger, which in real time, 40 million times every second has to make a decision about whether this collision is likely to contain an interesting object like a Higgs boson or dark matter particle. And it to do that very fast. [01:25:46] And the software algorithms in the past were quite relatively basic. [01:25:52] You know, they did things like measure momentos and energies of particles and put some requirements. So you would say if there's a particle with an energy above some threshold, then record this collision. But if there isn't, don't. [01:26:03] Whereas now the attempt to get more and more machine learning in the earliest possible stage, because cool at the stage of deciding whether we want to keep this data or not, but also even even maybe even lower down than that, which is the the point where there's this you know so well generally how the data is reconstructed as you start off with a digital a set of digital hits in your detector. So Channel saying, did you see something? Do you not see something that has to be then turned into tracks, particles going in different directions, and that's done by using fits that fit through the data points and then that's passed to the algorithms that then go, is this interesting or not? [01:26:37] Will be better if you could train and machine learning to just look at the raw hits, the basic real basic level information, not have any of the reconstruction done. [01:26:45] And it just goes and you can learn to do pattern recognition on this strange three dimensional image that you get. And potentially that's where you could get really big gains, because our triggers tend to be quite inefficient because they don't have time to do the full Whiz-Bang processing to get all the information out that we would like, because you have to do the decision very quickly. So if you can come up with some clever machine learning technique, then potentially you can massively increase the amount of useful data you record and, you know, get rid of more of the background earlier in the process. [01:27:16] To me, that's an exciting possibility because then you don't have to build a sort of you can get a gain without having to have to build any hardware or hardware that you need. [01:27:29] You need lots of new GPU farms, I guess. So hardware stops. [01:27:32] But the you know, I got to talk to you. I'm sort of I'm not sure how to ask, but you're clearly. An incredible science communicator, I don't know if that's the right term, but you're basically a younger Neil deGrasse Tyson with a British accent. [01:27:51] So and you've I mean, can you say where we are today? Actually, yeah. [01:27:56] So today we're in the Royal Institution in London, which is an old, very old organisation, has been around for about 200 years now. [01:28:04] I think maybe even I should know when it was founded sort of early 19th century, it was set up to basically communicate science to the public. [01:28:12] So it's one of the first places in the world where scientists, famous scientists would come and give talks. So very famously, Humphry Davy, who you may know of, who was the person who discovered nitrous oxide, is a very famous chemist and scientists also discovered electrolysis. So he used to do these fantastically, very charismatic speakers who used to peer here. There was a there's a big desk. They usually have it in the theatre. And he would do demonstrations to the sort of the the folk of London back in the early 19th century. [01:28:40] Michael Faraday, who I talked about, who is the person who did so much work, electromagnetism, he used he lectured here. He also did experiments in the basement. So this place has got a long history of both scientific research, but also in the communication of scientific research. So you gave a few lectures here. [01:28:55] How many to I've given you I've given a couple of lectures in this theatre before. [01:28:59] So I mean, that's so people should definitely go watch online. It's just the explanation of particle physics, although it's incredible. Like your your lectures are just incredible. I can't sing enough. So it was awesome. [01:29:12] But maybe can you say what did that feel like? What does it feel like to lecture here to talk about that? And maybe from a different perspective, more kind of like how the sausage is made is how do you prepare for that kind of thing? How do you think about communication, the process of communicating these ideas in a way that's inspiring to what I would say your talks are inspiring to the general audience. You don't actually have to be a scientist. [01:29:42] You can still be inspired without really knowing much of the you start from the very basics. So what's the preparation process? And then the romantic question is, what does that feel like to perform here? I mean, professionally? [01:29:56] Yeah, I mean the process. I mean, the talk that my favorite talk that I gave here was one called Beyond the Higgs, which you can find on the only role institutions YouTube channel, which you should go and check out. I mean, the channels got loads of great talks, a lot of great people as well. [01:30:09] I mean, that one I sort of given a version of it many times. So part of it is just practice. And actually I don't have some great theory of how to communicate with people. It's more just that I'm really interested and excited by those ideas and I talking about them. And through the process of doing that, I guess I figured out stories that work and explanations that when you say practice, you mean legitimately just giving just giving talks. [01:30:31] And I started off, you know, when I was a student doing talks and schools. And and I still do that as well some of the time and doing things. I've even done a bit of standup comedy, which was sort of went reasonably well, even if it was terrifying. And that's on YouTube as well. That's also I would I wouldn't necessarily recommend you check that out. [01:30:47] That's going to post the links several places to make sure people click on it. [01:30:51] Yeah, but it's basically I kind of have a story in my head. And I was you know, I kind of I have to think about what I want to say, usually have some images to support what I'm saying. And I get up and do it. And it's not really I wish there was some kind of I probably should have some proper process. [01:31:05] This is very it sounds like I'm just making up as I go along and I sort of oh, I think the fundamental thing they said, I think it's like I don't know if you know who a guy named Joe Rogan is. Yes, I do it. So he he's also kind of sounds like you in a sense that he is not very introspective about his process, but he's an incredibly engaging conversationalist. And I think one of the things that you and him share that I could see is like a genuine curiosity and passion for the topic. [01:31:39] I think that could be systematically, you know, cultivated. I'm sure there's a process to it. But you come to it naturally somehow. I think maybe there's something else as well, which is to understand something. There's this quote by Feynman, which I really like, which is what I cannot create. I do not understand. So like, I'm not I'm not particularly super bright. [01:31:59] Like, so for me to understand something, I have to break it down into its simplest elements and that, you know, and if I can then tell people about that, that helps me understand it as well. So I've actually I've learned a lot to understand physics a lot more from the process of communication because it forces you to really scrutinize the ideas that you're communicating and often makes you realize you don't really understand the ideas you're talking about. [01:32:22] And I'm writing a book at the moment, and I had this experience yesterday where I realized I didn't really understand a pretty fundamental theoretical aspect of my own subject. And I had to go and spend a couple of days reading textbooks and thinking about it in order to make sure that the explanation I gave captured the got as close to what was actually. [01:32:41] Happening in the theory, and to do that, you have to really understand it properly and then there's layers to understanding. It seems like the more there must be some kind of Fineman law, I mean, the more you the more you understand sort of the sympathy you're able to really convey the, you know, the the essence of the idea. So it's like this reverse the reverse effect. That's like the more you understand, the simpler the final thing that you actually convey. [01:33:13] And so the more accessible somehow it becomes. That's why Fineman's lectures are really accessible. It was just counterintuitive. Yeah. Although there are some ideas that. Are very difficult to explain how well or badly you understand, like, I still can't really properly explain the Higgs mechanism. [01:33:33] Yeah, because some of these ideas only exist in mathematics, really. And the only way to really develop an understanding is to go, unfortunately, to a graduate degree in physics. But you can get kind of a flavor of what's happening, I think. [01:33:49] And it's trying to do that in a way that isn't misleading, but was also intelligible. [01:33:53] So let me ask then the romantic question of what do you is the most perhaps an unfair question? What is the most beautiful idea in physics? One that fills you with or is the most surprising, the strangest, the weirdest. There's a lot of different definitions of beauty, and I'm sure there's several for you. But is there something that just jumps to mind that you think is just especially. I mean, wow, beautiful. There's a specific thing in a more general thing, so maybe the specific thing first, which I can come across as an undergraduate, I found this amazing. [01:34:30] So this idea that the forces of nature, electromagnetism, the strong force, the weak force, they arise in our theories as a consequence of symmetries. [01:34:41] So symmetries in the laws of nature, in the equations essentially that used to describe these ideas, the process whereby theories come up with these sorts of models, as they say, imagine the universe obeys. This particular type of symmetry is a symmetry that isn't so far removed from a geometrical symmetry like the rotations of a cube. It's not you can't think of it quite that way, but it is sort of a similar sort of idea. And you say, OK, if the universe respects the symmetry, you find that you have to introduce a force which has the properties of electromagnetism or different symmetry. [01:35:15] You get the strong force or different symmetry, you get the weak force. So these interactions seem to come from some deeper. It suggests that they come from some deeper symmetry principle. I mean, depends a bit how you look at it, because it could be that we're actually just recognizing symmetries in the U.S. But there's something rather lovely about that. I mean, I suppose the biggest thing that makes me wonder is actually if you look at the laws of nature, how particles interact when you get really close down, they basically pretty simple things. [01:35:41] They bounce off each other by exchanging, you know, through force fields and they move around in very simple ways. And somehow these basic ingredients, these few particles that we know about in the forces creates this universe, which is unbelievably complicated and has things like you and me in it and, you know, the earth and stars that make matter in their cause by from the gravitational energy of their own. Bulc that then gets sprayed into the universe that forms other things. [01:36:05] I mean, the fact that there's this incredibly long story that goes right back to, you know, the can we can take this story right back to, you know, trillionth of a second after the big bang. And we can trace the origins of the stuff that we're made from and are all ultimately comes from these simple ingredients with these simple rules. And the fact you can generate such complexity from that is really mysterious, I think, and strange. And it's not even a question that physicists can really tackle because we are sort of trying to find these really elementary laws. [01:36:35] But it turns out that going from elementary laws and a few particles to something even as complicated as a molecule becomes very difficult. It's like going from molecule to a human being is a problem that just, you know, can't be can't be tackled, at least not at the moment. [01:36:50] So, yeah, the emergence of complexity from simple rules is so beautiful and so mysterious. And there's no we don't have good mathematics to even try to approach that emergent phenomena. That's why we have chemistry and biology and all the other subject. [01:37:07] Yeah, I don't think I don't think there's a better way to end it. Harry, I can't. I mean, I think I speak for a lot of people that can't wait to see what happens in the next five, 10, 20 years. Do I think you're one of the great communicators of our time? So I hope you continue that and I hope that grows. And definitely a huge fan. So it was an honor to talk to you today. [01:37:30] Thanks so much. [01:37:31] Thanks very much. Thanks for listening to this conversation with Harry Cliff and thank you to our sponsors Express, VPN and Kashyap. Please consider supporting the podcast by getting Express VPN and Express Report.com Flex Pod and downloading cache app and using Culex podcast. Enjoy this podcast. Subscribe on YouTube, review it with five stars, an Apple podcast supporter and patron, or simply connect with me on Twitter, Àlex Friedemann. And now let me leave you with some words from Harry Cliff. [01:38:06] You and I are leftovers, every particle in our bodies is a survivor from an almighty shootout between matter and antimatter that happened a little after the Big Bang. In fact, only one in a billion particles created at the beginning of time have survived to the present day. Thank you for listening and hope to see you next time.

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