experimental tests of continuous symmetries gerco onderwater kvi/rijksuniversiteit groningen, the...

30
Experimental Tests of Experimental Tests of Continuous Symmetries Continuous Symmetries Gerco Onderwater Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlan KVI/Rijksuniversiteit Groningen, The Netherlan

Upload: toby-cain

Post on 29-Dec-2015

216 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Experimental Tests ofExperimental Tests ofContinuous SymmetriesContinuous Symmetries

Gerco OnderwaterGerco OnderwaterKVI/Rijksuniversiteit Groningen, The NetherlandsKVI/Rijksuniversiteit Groningen, The Netherlands

Page 2: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Continuous Symmetries

Are related to space and time. Translations and rotations in space, and time can take any value, hence they are continuous.

A physics law is said to be symmetric under such transformations if it does not change, i.e. the law is invariant.

Page 3: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Noether's Theorem

Continuous symmetry ↔ conservation law

Invariant under Conservation of

(1) time translation energy(2) space translation momentum(3) rotation angular momentum(?) boost Lorentz generators

Page 4: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

How to Test?Two possibilities:

(1) Test that a process is the same when occuringhere and there, now and then, etc.

(2) Test the associated conservation law explicitly

Important constraint:

the trial system is isolated from external influences!

Page 5: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

(1) Time Invariance(1) Time Invariance&&

Energy ConservationEnergy Conservation

Page 6: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

What is Energy?

Energy can be defined as the capacity for doing work.

It may exist in a variety of forms and may be transformed from one type of energy to another.

Transformations constrained by conservation principle

One way to state this principle is "Energy can neither be created nor destroyed". Another approach is to say that the total energy of an isolated system remains constant.

E1=-E2 or E1+E2=C: this we can test!

Page 7: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Types of EnergyA complete test of energy conservation would require the demonstration that each of the kinds of energy below are equivalent

nuclear electric

potential kinetic thermal

mass chemical

In the end, all energy is kinetic or potential

Note that potential energy can be sub-divided according to each of the four known forces

Page 8: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Joule's Paddlewheel Exp't

[Philos. trans. Royal Soc. London, 140, pp. 61-82 (1840)]

Classical experiment to showequivalence of 3 types of energy

gravity – kinetic - thermal

Page 9: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Photoelectric EffectEmission of electrons under illumination. The electron kinetic energy increases with decreasing photon wavelength, the rate with intensity.

Demonstrates equivalence ofquantum and kinetic energy

Page 10: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Classic LawsOther observation-based laws, effects and relations that support continuous symmetries

Bernouilli Volt Ohm KirchhoffAmpere Biot-Savart Coulomb BraggCharles Curie-Weiss Doppler FaradayGauss Joule Keppler Le Chatelier Lenz Mach Maxwell Meissner Newton Wien Planck KelvinRayleigh-Jeans Snell Stefan-Boltzmann

and probably some ...

Page 11: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Watt Balance

hehheRK

iR

KnfV

V

SI

UI

mgv

electrical

mechanicalz

ImgF

zv

zdt

dz

dt

dU

KJ

K

J

z

z

/4)/()/2(

/

/

}/{

}{

222

2

Electrical standard of kgChange SI to QM standard

HW

Page 12: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

When a DC voltage is applied to a Josephson junction,

an oscillation of frequency                             occurs at the junction.

Josephson junction standards can yield voltages with accuracies of one part in 1010. NIST has produced a chip with 19000 series junctions to measure voltages on the order of 10 volts with this accuracy.

Josephson Voltage Standard

Page 13: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Quantum Hall resistance standard

2/ iehRH

Page 14: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Quantum Hall Array Standard (QHARS)

1cm 1cm100 standard

Page 15: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Metrological triangle

new standard ?

Page 16: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Beta Decay Mystery

Beta energy expected to be mono-energetic A continuous spectrum was observed

Two explanations(1) energy non-conservation(2) new invisible particle

Did not fulfill closed system requirement

Page 17: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Time InvarianceSearch for time variation of reaction rate

Weak InteractionOklo natural reactor: |ĠF/GF|<1x10-11/year

EM InteractionQuasar H spectra: = -(0.7±0.2)×10-5 for 0.5<z<3.5Proton/electron mass: = (2.0±0.6)x10-5 / 12 Gyr

Strong InteractionRb/Cs = -(0.9±2.9)x10-15 /year

This will be discussed in more detail later in the course

Eur. Phys. J. A 8, 137–140 (2000) Phys. Rev. Lett. 96, 151101 (2006) Phys. Rev. Lett. 87, 091301 (2001) Phys. Rev. Lett. 92, 230802 (2004)

Page 18: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Energy in Quantum Mechanics

The uncertainty principle states that Et≥ħ

Does this mean energy conservation may beviolated (briefly)?

HW: wrong question

Page 19: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

(2) Spatial Invariance(2) Spatial Invariance&&

Momentum ConservationMomentum Conservation

Page 20: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

What is Momentum?

Momentum can be though of as the tendency ofan object to continue in its direction of travel

Classically: p = mvRelativistic: p = mvMassless: p = E/c = h/Quantum: p = -iħ

Change requires an external force

Page 21: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Every Day Life

Page 22: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Compton Effect

The increase in wavelength of a photon scattering of an electron

Demonstrates that photons carryenergy and momentum

= h/mec ( 1-cos) + 1

Page 23: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

e+e- → 2Ps →1 : E=2me p=E/c ≠ pPs=0 FORBIDDEN

Ps →2 : E=me p+p=0 ALLOWED

Collinearity = (relativistic four) momentum conservation

Phys. Rev. 77, 205–212 (1950)

Page 24: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

(3) Rotation Invariance(3) Rotation Invariance&&

Angular MomentumAngular MomentumConservationConservation

Page 25: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

What is Angular Momentum?

Angular momentum is the measure of rotation around some fixed point in space(also includes spin)

Classically: L = rxpRelativistic: L = rxpMassless: L = SQuantum: L = -iħrxp

Change requires an external torque

Page 26: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Kepler's Second Law

A line joining a planet and its star sweeps out equal areas during equal intervals of time

Tested in solar system observations

Page 27: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Michelson-MorleyClassic experiment to test isotropy of c

Modern version: compare flaser,xy vs time of day (2 rotation)

c/c = (2.6±1.7)x10-15

Phys. Rev. Lett. 21, 020401 (2003)Phys. Rev. D 67, 056006 (2003)

Page 28: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Isotropy of -DecayMeasure differential decay rate and see if it varies with orientation w.r.t. some fixed frame (stars)

() = [ 1 + 1cos() +2cos(2) ]

< 1.6x10-7 < 2x10-6

Phys. Rev. D 14, 1 (1976)

Page 29: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Isotropy of MassMeasure Zeeman splitting for 3He(J=½) and 21Ne(J=3/2) (Hughes-Drever experiments)

Search for orientation-dependent binding energy = inertial mass

Lowest order: quadrupole splitting(so 3He is not sensitive)

|E/E| < 1.6x10-26

Phys. Rev. Lett. 14, 1541 (1989)Phys. Rev. Lett. 64, 2261 (1990)

Page 30: Experimental Tests of Continuous Symmetries Gerco Onderwater KVI/Rijksuniversiteit Groningen, The Netherlands

Pion Decay

Best limit of angular momentum conservation in weakinteraction comes from (→e)/(→) ~ 10-4

The small factor is “unexpected” in view of (giant) phase for electron decay, but…Axial vector delivers wrong helicity (need l=1 for angular momentum conservation)

More: absence of pseudo scalar (P) coupling in WI

+

+