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Physics beyond the Standard Model from molecular hydrogen; Part I

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Presentation on theme: "Physics beyond the Standard Model from molecular hydrogen; Part I"— Presentation transcript:

1 Physics beyond the Standard Model from molecular hydrogen; Part I
ALMA VLT HST Effelsberg Lasers Wim Ubachs Vrije Universiteit Amsterdam PSAS 2016 Jerusalem, 23 May 2016

2 Varying Constants of Nature ?
Coupling constants are free parameters in Standard Model But cannot be varied at will Bekenstein – Barrow – Flambaum : consistent models 1) Coupling to matter Variation on cosmological time scales “Connection to Dark Energy scenarios” 2) Coupling to environment -> “chameleons” Dependence on local density Dependence on gravity

3 Lab QSO Empirical search for a change in m
Compare H2 in different epochs Lab today QSO 12 Gyr ago nm ~ nm Cosmological redshift Practical: atmospheric transmission only for z>2

4 H2 molecule 2pp 2ps H H2 Blue-shifted from Lyman-a
(1s)2- (1s)(2p); threefold 2p orbitals 2pp 2ps H H2 X1Sg+ - (2ps) B1Su+ X1Sg+ - (2pp) C1Pu Blue-shifted from Lyman-a Doubly degenerate

5 H2 dipole-allowed spectrum
Blue-shifted from Lyman-a 2pp 2ps H H2 Theodore Lyman H2, Lyman en Werner BANDS ~ nm Extreme Ultraviolet Wavelengths

6 “Sensitivity” Perturbations

7 H2 laboratory wavelengths
The Amsterdam “XUV-laser” XUV-laser excitation P(3) C-X (1,0) R(0) B-X (9,0) line Ubachs, Phys. Rev. Lett. (2004) Reinhold et al, Phys. Rev. Lett. (2006) Salumbides et al, Phys. Rev. Lett. (2009) For HD Ivanov et al., Phys. Rev. Lett. (2008)

8 Soleil VUV Fourier-Transform Spectrometer
HD

9 >160 lines measured at ~ 5 x 10-8 Some lines at < 1 x 10-8

10 VLT – UVES Paranal, Chili Keck – HIRES Hawaii

11

12 Various systems observed

13 Analysis method: “comprehensive fitting”
Produce molecular fingerprint li – set of accurate wavelengths fi – set of line oscillator strengths (from ab initio theory) Gi – set of damping coefficients (from ab initio theory) Astrophysical conditions b – Doppler width parameter z – red shift NJ – column densities Fit equation onto spectrum “Treat” HI and metal lines Multiple velocity components (?) Ki – set of sensitivity coefficients

14 The best system: J2123-005 at zabs=2.05
Unique spectrum from Keck; Resolution ; seeing 0.3” Spectrum from VLT; R=54000; seeing 0.8”; better SNR 37 panels, 3071 – 3421 Å ~100 H2 + 7 HD lines Keck: Dm/m = (5.6 ± 5.5stat ± 2.9syst) x 10-6 VLT: Dm/m = (8.5 ± 3.6stat ± 2.2syst) x 10-6

15 Q1441+272 ; the most distant zabs = 4.22 ; 1.5 Gyrs after the Big Bang
Systematic analysis Phys. Rev. Lett. 114, (2015)

16 Status |Dm/m| = (3.1  1.6) x 10-6 W. Ubachs, J. Bagdonaite, E.J. Salumbides, M.T. Murphy, L. Kaper Search for a drifting proton-electron mass ratio from H2 Rev. Mod. Phys. 88, (2016)

17 Satelite-Based observations
Cosmic Origins Spectrograph Hubble Space Telescope Dependence of m on gravitational field Spectrum of GD-133 and GD29-38 White Dwarf stars H2 in VUV In search for the chameleon scenario (local conditions)

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19 Contributions of many lines in the B-X Lyman system
l ~ nm High temperatures High v populated Franck-Condon factors

20 Dependence of Dm/m on gravitational field
Invoke partition function: Invoke intensities (1500 lines): Fit T and Dm/m GD133: Dm/m = (-2.7 +/- 4.7) x 10-5 GD29-38: Dm/m = (-5.9 +/-3.8) x 10-5 Bagdonaite et al., Phys. Rev. Lett. 113, (2014)

21 CO A1P-X1S+ electronic bands
POSTER CO A1P-X1S+ electronic bands In J at z=2.69

22 Search for higher sensitivity molecule
What should you look at ? Search for higher sensitivity molecule Calculations Extreme shifters

23 Methanol: the extreme shifter
MHz; K=-1 MHz; K=-1 MHz; K=-33 MHz; K=-7

24 PKS-1830-211 “molecular factory” A Stringent Limit on a Drifting
Effelsberg Radio Telescope PKS “molecular factory” at z= (7.5 Gyrs look-back) A Stringent Limit on a Drifting Proton-to-Electron Mass Ratio from Alcohol in the Early Universe Bagdonaite, Jansen, Henkel, Bethlem, Menten, Ubachs, Science 339 (2013) 46 K=-33 K=-1 K=-7

25 PKS1830-211; lensing, blazar, time-varying
Radio-loud quasar “Blazar” Intervening galaxy with cold methanol

26 Result from three telescopes
IRAM-30m Chajnantor, Chile 5 km altitude 160 GHz 261 GHz

27 HD+ ions in a trap; measurement of (8,0)
Look for loss of HD+ 750 Be+ 40-85 HD+ Signal detection by REMPD 782 nm + 532 nm 313 nm

28 HD+ spectrum Theory 782 nm Experiment
J = 4 HD+ spectrum S = 2 J = 3 J = 2 J = 1 J = 0 F = 1 S = 1 J = 3 J = 2 J = 1 v = 8, L =2 Theory S = 0 J = 2 F = 0 S = 1 J = 1 J = 2 J = 3 782 nm J = 5 S = 2 J = 4 J = 3 J = 2 J = 1 F = 1 S = 1 J = 4 J = 3 v = 0, L =3 J = 2 Experiment S = 0 J = 3 F = 0 S = 1 J = 2 J = 3 J = 4 Experiment: 383,407,177.38(41) MHz Theory*: 383,407, (15) MHz *Korobov, Hilico, Karr, Phys. Rev. A 89, (2014) Biesheuvel et al. (Nature Comm. 2016)

29 Thanks & Acknowledgement
MingLi Niu Paul Jansen Julija Bagdonaite Mario Dapra Edcel Salumbides Isabelle Kleiner Jeroen Koelemeij Jurriaan Biesheuvel HD+ Michael Murphy Karl Menten Nissim Kanekar


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