Cosmic rays and how a Bristol Physicist won the Nobel Prize Dr Helen Heath.

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Cosmic rays and how a Bristol Physicist won the Nobel Prize Dr Helen Heath

Transcript of Cosmic rays and how a Bristol Physicist won the Nobel Prize Dr Helen Heath.

Page 1: Cosmic rays and how a Bristol Physicist won the Nobel Prize Dr Helen Heath.

Cosmic raysand how a Bristol Physicist won the Nobel Prize

Dr Helen Heath

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1788

http://books.google.co.uk/books?id=by5EAAAAcAAJ

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100 years of Cosmic Rays

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NASA TV

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What are cosmic rays

• Primary Cosmic rays• 85% protons• 12% helium nuclei (alpha particles)• 3% heavier nuclei• 2% electrons

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http://www.phys.uu.nl/~thooft/quarks.gif

Baryons

Mesons

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Particle Energy(MeV) v year

1900 1920 1940 1960 1980 2000 20201

10

100

1000

10000

100000

1000000

10000000

First Cy-clotron

BevatronAntiproton

LHC

Mass of lightest “new particles”

Natural Radioactivty

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Cecil Frank Powell

• Nobel Prize 1950

“for his development of the photographic method of studying nuclear processes and his discoveries regarding mesons made with this method.

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The Start of Big Physics?

• “These developments in international collaboration formed an essential background to the setting up of large international laboratories such as CERN”

D.H.Perkins

40 years of Particle Physics Conference

Bristol July 1987

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Sub-atomic particles

• Nucleus• Protons • Neutrons

• Electrons• First antimatter particle – positron• Photons

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Yukawa

• Proposed a field theory of nuclear forces.• Field theory requires field quanta.

• We can estimate the mass of such a quanta from the Uncertainty Principle• E t ≈ h (h=6.63x10-34Js)• t ≈10-15/c ≈ 0.3x10-22s• E ≈ 2.2x10-11J• E = mc2 m=0.24 x 10-27 kg=0.14mp

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Mesons

• If Yukawa’s theory was correct • there must be a field particle

• The hunt was on for a meson• Today we use meson to mean a combination

of a quark and an antiquark• Originally it was a particle with a mass

between the proton and electron• Mesos – Intermediate

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(Modern Aside)

• Mass is unexplained • Proposed Higgs

Mechanism• Requires Higgs Field• ..and therefore the

Higgs boson

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Experimental techniques

• Cloud Chambers• Bubble Chambers• Emulsions• Solid detectors

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Cloud Chamber

• The discovery of the positron• Carl D. Anderson – Physical Review 1933

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Bubble Chamber

©CERN photo

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Cecil Powell

• Cecil Powell started an autobiography which can be found at• http://www.phy.bris.ac.uk/history.html

• He succeeded academically winning a scholarship to Judd School and then moving on to Sidney Sussex Cambridge

• From an early age he was an enthusiastic, if not always, talented investigator.

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After Cambridge

• Nearly became a teacher

• Research student at Cambridge • Supervised by Wilson

• Recruited by Tyndall to Bristol in 1928

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The emulsion technique

• Cloud chambers and bubble chambers need to be photographed

• Emulsions are continuously active• Emulsions are also rather portable

• Important for early observatories & balloons

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http://www.imcce.fr/phemu03/Promenade/pages5/545.html

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Photographic Emulsion

• Grains of silver bromide suspended in gelatine.

• Light causes changes to the silver bromide.

• Developer changes the affected grains to silver

• Fixer removes the remaining silver bromide

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Powell’s research group

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The pion

• In 1936 C. Anderson and S Neddermeyer observed negatively charged particles with mass intermediate between that of the proton and the electron• Initially called mesotrons• Renamed the mu-meson in 1947

• Now mesons are a subset of hadrons • The mu meson is a lepton

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Measuring energies

• Energy loss in the Emulsion is approximately continuous.• The range of a particle depends on its energy

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Double meson events

• Seen in events from the Jungfrau Joch• The second meson has a range of 600 m

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Interpretation

• In Double meson events one meson decays to another

• - -

• Since the pion has stopped all the kinetic energy of the decay products comes from the change in mass• Pion mass =139.6 MeV/c2

• Muon mass = 105.7 MeV/c2

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After the Nobel Prize• Powell continued

to work with emulsions

• Left is the first example of a Kaon decay to three pions

• Work switched to balloons rather than mountains.

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Modern Cosmic Ray Work

LHC Energies

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Open Question

• Origin of very energetic cosmic rays

• GZK –Cutoff

(Griesen-Zatsepin-Kuzmin)

Cronin, J. W., 1999, Cosmic Rays: the most energetic particles in the universe, RvMA 71, 165–172

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Sparse Array – Large area

HiSPARC project High School Project

on Astrophysics Research with Cosmics

>100 detector across

The Netherlands

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HiSPARC – school detector

Students build their own detector

And place it on top of the roof of the school

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