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The must fundamental constituents of matter Physics 100 Chapt 26.

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Presentation on theme: "The must fundamental constituents of matter Physics 100 Chapt 26."— Presentation transcript:

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2 The must fundamental constituents of matter Physics 100 Chapt 26

3 Anaximenes Anaximenes ~600BC All types of matter are formed from different combinations of: Earth Air Fire Water

4 Closer to home Earth Wind Fire Water Elements

5 Anaximenes idea Good point: Economical –All of matter reduced to 4 easy-to-remember components Bad point: Wrong –Alchemists (including Isaac Newton) tried for centuries to changing one chemical element into another with no success

6 Enter Mendeleev All matter is comprised of different combinations of (now 92) different chemical elements Good point Correct; successfully predicted the existence of Scandium, Gallium & Germanium Bad point Uneconomical; 92 basic constituens

7 Rutherford All elements are constructed from 3 basic particles: electrons neutrons protons Feel the strong force & are heavy  hadrons Doesn’t feel the strong force & is light  lepton

8 The “elementary particles” circa 1935 Categoryparticlesymbolchargemc 2 strongelectricweak Leptons electron e-e- 0.511 MeV noyes neutrino 0~0no yes Hadrons proton p+1 938.3 MeV yes neutron n0 939.6 MeV yes Light photon  00noyesno Economy is restored Forces felt

9 These “good” times didn’t last long

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11 Paul Adrien Maurice Dirac 1902 - 1984 Combined relativity & Quantum Mechanics

12 p = mV x p x = mV x E = 1/2 mv 2 p y = mV y y Pre relativity p x can be + or - E is always +

13 p = mV x p x = mV x E = mc 2 2 2 () ± p y = mV y y p x can be + or - E also can be + or - Post relativity:

14 QM waves: =h/p f=E/h Pre relativity: p = m 0 v (v =p/m 0 ) E = 1/2 m 0 v 2 =p 2 / 2 m 0 = h/p  can be + or  f=p 2 / 2 m 0 h  always +

15 QM waves: =h/p f=E/h after relativity: p =  m 0 v (v =p/m 0 ) E 2 = (mc 2 ) 2  E= ± mc 2 = h/p  can be + or  f=  can be + or   mc 2 h

16 Negative wavelength : wave in backward direction. Negative frequency : wave backward in time????

17 What does it mean to move backwards in time?

18 backward time motion          t B when viewed forward in time:  LR : C : P

19 When antimatter comes in contact with matter, what happens?

20 -+- + - +    

21 Anti-hydrogen p + Anti-hydrogen atoms are made routinely at the CERN laboratory in Switzerland. It is found to have the same size and allowed energy levels as ordinary hydrogen

22 Anti-Carbon + + + + + + antielectrons antineutrons antiprotons Although it would be impossibly difficult to make anti-atoms more complex than anti- hydrogen, it is in principle possible

23 CP Violation: Asymmetry matter anti- matter Big Bang matter- antimatter symmetric all matter no antimatter

24 Our research Where did all the anti-people go???

25 Include anti-particles in our list Categoryparticlesymbolchargemc 2 symbolcharge Leptons electron e-e- 0.511 MeV positron e+e+ +1 neutrino 0~0 anti- neutrino 0 Hadrons proton p+1 938.3 MeV anti- proton p neutron n0 939.6 MeV anti- neutron n0 Light photon  00  0 anti-particle particle

26 Quantum Electro-Dynamics (QED) Combined Relativity, Quantum Mechanics and Photons into one single theory Richard FeynmanJulian Schwinger Shinichiro Tomonaga

27 QED explains action-at-a-distance

28 QED is a fabulously accurate theory QED theory measure Strength of electrons magnetic field:

29 Ideas of QED  strong nuclear force Hideki Yukawa  Short range (10 -15 m) of the strong nuclear force: predicts existence of a “  ” particle  M  c 2  140 MeV 1935

30 Look for  in cosmic rays

31 “Spark chamber” tracks

32  + and  – particle discovered in cosmic rays m  + c 2 = m  - c 2 = 106 MeV Near expectations for Yukawa’s  Experiments show that the  + &  - do not feel the Strong Nuclear Force and, therefore, cannot be Yukawa’s  the  + &  - are additional leptons (i.e. like the e + & e - but with larger mass)

33 Yukawa’s  finally discovered in 1947 In fact there are 3 of them:  +  M  + c 2 = 139.6 MeV  0  M  0 c 2 = 135.0 MeV  -  M  - c 2 = 139.6 MeV Anti- particles Photographic emulsion

34 “Atom smashers”

35 Inside the accelerator tunnel

36 e + e - collider

37 Belle Detector

38 Electronic detectors

39 Fermilab (near Chicago) 2 km detector

40 Inside a Fermilab Tunnel

41 Biggest of all is in Europe ~5 miles

42 Detectors

43 Neutrino interacts in a Bubble Chamber

44 Leptons (circa 2005) anti-particle particle namesymbolchargemc 2 namesymbolcharge electron ee 0.511 MeV positron ee +1 electron neutrino e 0~0 anti-elec neutrino e 0 muon  +1 105.7 MeV anti- muon  +1 muon- neutrino  0~0 anti-mu neutrino  0 tau  1876 MeV anti- tau  +1 tau- neutrino  0~0 anti-tau neutrino  0

45 1950’s & 1960’s, Many other particles are discovered   p  - M=1116MeV

46 K 0 “meson”      K 0     - M=498 MeV

47 Two classes of hadrons Baryons (p, n, , …..) ultimate decay products include a proton Mesons ( , K, …) ultimate decay products e’s,  ’s & ’s Both baryons & mesons feel the Strong Nuclear Force

48 Lots of baryons have been discovered

49 & even more mesons

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51 The elementary particle chart revisited Economy is lost!! 6 leptons: e e ;   ;   (+ 6 anti-leptons) Categoryparticlesymbol Leptons electron e-e- neutrino Hadrons proton p neutron n 1935 NOW hundreds of hadrons + anti-hadrons

52 Elementary Particle Zoo Lepton House Electrons, Muons, Taus, & lots of neutrinos Hadron Savannah 100’s of Baryons, Latest new Mesons +anti particles galore & lots of photons Special today: live pions being exhanged proton neutron


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