Gravitation im Labor

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“Testing Gravity” Hinrich Meyer Uni. of Wuppertal with W. Bartel, B. Löhr, E. Lohrmann and S. Schubert Gravitation im Labor

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Gravitation im Labor. “Testing Gravity” Hinrich Meyer Uni. of Wuppertal. with W. Bartel, B. Löhr, E. Lohrmann and S. Schubert. Outline:. 1.) Astronomy and Astrophysics. 2.) Experiments in the laboratory. anno 1632. Hamlet Act1, scene5. The are more things in heaven and earth, - PowerPoint PPT Presentation

Transcript of Gravitation im Labor

Page 1: Gravitation im Labor

“Testing Gravity”

Hinrich MeyerUni. of Wuppertal

withW. Bartel, B. Löhr, E. Lohrmann

and S. Schubert

Gravitation im Labor

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1.) Astronomy and Astrophysics

2.) Experiments in the laboratory

Outline:

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anno 1632

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The are more things in heaven and earth,Horatio,

Than are dreamt of in your philosophy

Hamlet Act1,

scene5

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BBN successfully describing light element abundances in

the universeall but H

missing baryon problemFukugita, Peebles 1988

(BUT!!!!!)

Q: how much matter there is in the Universe???

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XMM NewtonESA X-RAYSatellite

observingmissing

baryon fractionsolved??

Text

also spectral lines from intergalactic clouds

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virial lawE(kin)=-1/2E(pot)

Helvetica Physica Acta1933

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Vera Rubin 1970, with K. Ford

Rotation curves a generalphenomenon

Andromeda M31

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Spiral Galaxies

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Scarpa, Gilmozzi, et al. 2006, globular clusters

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In the solar system??

at least two dramatic effects

a: “Pioneer” anamoly

b: “fly by” effect

again seem to be ruled bya(0) about cH!!

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F(grav)=GmM/r2

Newtons law

rules all bound systems in the universe

a: change M , by introducing CDM

b: change accel. by introducing a(0) at very small accel. a MONDactually, a(0) is about cH

c: adding an Yukawa like term at very small distance

d: consider G to be time dependent

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“MOND”Milgrom 1983nonrelativistic

“TeVeS”Bekenstein 2004

relativistic extension

Proposals, to change Newtons Law

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Sanders, Noordmeerearly type disks

2007

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dwarf spheroidals

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Sanders, 1996

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MOND works:however

needsNeutrinos with mass

seeZhao 2007

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Thus, it is my personal opinion – and I am the only one responsible for it if proved wrong-- that if Newtonian dynamics fails below a0, this should be true irrespectively of the total field and one should be able to observe MOND effect also here on earth. For instance, I think a refined version of the Cavendish experiment studying gravitational forces in the horizontal plane should detect MOND effects.

R. Scarpa 2006

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Laboratory experiments

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fieldmass560kg

now only5-40kg

thesis work bySchurr, Walesh, Schumacher,

Kleinevoss1992 - 2002with H. Piel

Univ. of Wuppertal

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db =df const

const=10-9

(m/kHz)thesisH. Walesch

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2006recent “G” results

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Earthquake signal in GRAVI

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TextTextText

Noisenicely

Gaussian,very

crucial

frequencyvs.

time

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“Gravi” at DESY works!!! (18.6.2008)127Hz in 22GHz (1/10 nm)

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Goals with “GRAVI” at DESY

a: measurements in theMOND region

b: accurate determinationof big “G”

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blue line prefered by astrophysical considerations

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Schlamminger et al.Zürich

G measurment

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Eötwash

AdelbergersgroupSeattle

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equivalence principle

testSchlamminger et

al.2008

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fascinating timestesting

GRAVITYin the lab

I like to thank DESYfor unbureaucratic

support