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Title: Geophysical tests of gravitational physics with superconducting gravimeters


1
Geophysical tests of gravitational physics with
superconducting gravimeters
  • Sachie Shiomi
  • Space Geodesy Laboratory,
  • Department of Civil Engineering,
  • National Chiao Tung University,
  • Hsinchu, Taiwan

2
Contents
  • Introduction
  • Superconducting Gravimeters (SGs)
  • Examples of applications to gravitational physics
  • The global network of SGs
  • Application 1 Testing the universality of
    free-fall
  • Application 2 Searching for dilatonic waves
  • Summary

3
Superconducting gravimeter (SG)
  • Sensitive and stable at low frequencies

1 m
Hsinchu SG, operated by NCTU and CMS
4
Working principle
Gravimeter Sensing Unit
  • Sphere is levitated by magnetic fields induced
    by currents in the superconducting levitation
    coils.
  • Motion of the sphere is monitored by capacitor
    plates.

F 2.5 cm
4.2 K
J. M. Goodkind, Review of Scientific Instruments
70 (1999)
5
Applications to gravitational physics
  • Earliest work (1976)
  • Search for evidence of a preference frame
  • (Warburton and Goodkind, Astrophysical Journal,
    1976.)
  • More recent works, e.g.
  • Test of the inverse-square law
  • (Goodkind et al PRD 1993, Baldi et al PRD,
    2001)
  • Measurement of gravitational constant G
  • (Baldi et al PRD, 2005)

6
The GGP network
  • The Global Geodynamics Project (GGP) network of
    superconducting gravimeters (1997) about 25
    operating sites.
  • To study geophysical signals in global nature,
    i.e. oscillation of the inner core, polar motion
    and wobbles.

D. Crossley, Journal of Geodynamics 38 (2004)
7
D. Crossley
8
Applications of the global network to
gravitational physics
  • We investigate possible applications of the GGP
    network to study gravitational physics.
  • One of such applications is testing the
    universality of free-fall.

9
Testing the universality of free-fall
10
Universality of free-fall
  • Every material (point mass) in a given external
    gravitational field falls at the same rate.

http//www.endex.com/gf/buildings/ltpisa/ltpnews/p
hysnews1.htm
11
Motivations of testing the universality
  • Fundamental principle
  • It should be tested as precisely as possible.
  • New physics?
  • Theories towards the unification of the four
    fundamental forces predict new interactions that
    violate the principle.

12
Proposed new forces (spin-independent)
Motivated by Bosons (Spin) Mass Charge References (year)
Conservation of baryon charge Vector bosons (1) massless B Lee and Yang (1955)
Supersymmetry U-bosons (1) Massive (very light) B, Iz Fayet(1986)
String theory Dilatons(0) Dilatons(0) Moduli(0) massive massless massive (millimeter range) Ordinary matter B, Iz, E Ordinary matter Fujii(1971)Taylor and Veneziano (1988) Damour and Polyakov(1994) Dimopoulos and Giudice(1996)
Composition dependent
13
Modification of Newtons law
V(r)
Yukawa-potential type
14
Current limits
Fischbach and Talmadge, The Search for
Non-Newtonian Gravity (Springer-Verlag, 1999)
15
The necessity of variety in experimental
approaches
  • The universality has to be tested for various
    putative charges, using different kinds of test
    bodies, at different ranges.
  • To confirm experimental results, it should be
    tested by at least two different experimental
    methods.

16
The concept
Sun
  • If the universality were violated, the inner core
    would move relative to the rest part of the
    Earth.
  • Surface gravity changes

17
Test bodies inner core and the rest
  • Chemical composition
  • Density kg m-3
  • Inner core (iron, nickel) 13000
  • The rest (silicon oxides) 5400
  • Gravitational binding energy
  • Inner core -3.7 10-11
  • The rest -4.2 10-10

18
Best observation points
  • In Spring and Autumnal equinox points on the
    equator
  • In Summer and Winter solstices on Tropic of
    Cancer or Capricorn

19
Equation of motion of the inner core
Gravitational stiffness
Damping effect
Violation effect
S. Shiomi, Physical Review D 74, 027101(2006)
20
Forced oscillation
When the damping coefficient (k) is sufficiently
small
Surface gravity changes
10-12 ms-2
21
Expected sensitivity
Current limits a few parts in 1013 nearly four
orders of magnitude improvement is necessary.
22
Improving the sensitivity (1)
  • Carrying out coincidence measurements at two
    observatories located opposite side of the Earth
    near the equators.

23
Improving the sensitivity (2)
  • Development of the data analysis method to
    extract weak signals.
  • e.g.
  • Non-Linear Damped Harmonic Analysis method (S.
    Rosat et al, J. Geodyn. in press)

24
Summary expected signals
Direction along the Earth-Sun line
Frequency once per day once per year
25
Future works
  • Improving noise reduction methods
  • Identification of environmental noise
  • Data analyses to extract weak signals
  • Figuring out the optimum scheme of global
    observations
  • e.g. coincidence measurements
  • Improvements of the sensitivity of SGs
  • Application of elaborate Earth models

26
Conclusions
  • The universality of free-fall can be tested using
    a superconducting gravimeter installed near the
    equator to 10-9.
  • Some improvements can be expected from global
    observations and applications of advanced data
    analysis methods.

27
Search for composition-dependent dilatonic waves
28
Introduction
  • String theory predicts the existence of relic
    background of the dilaton (a scalar partner of
    the graviton).
  • Ordinary macroscopic test masses have dilatonic
    charges, which depend on their internal
    compositions.
  • The response of the test masses to dilatonic
    waves is non geodesic.

M. Gasperini, Phys. Lett. B 470, 67 (1999)
29
The concept
30
Estimation of upper limits (1)
Spectrum of the displacement ( l ) at resonance
Dimensionless energy density for massless dilaton
31
Estimation of upper limits (2)
From residual gravity data, an upper limit on the
displacement is 1.1 10-4 m Hz-1/2 at 7 10-5
Hz. (S. Rosat et al, J. of Geodyn. 38 (2004))
Effective viscosity 10-3 1012 Pa s (R.A.
Secco, A Handbook of Physical Constants)
S. Shiomi, Geophysical search for dilatonic
waves (submitted in 2007)
32
  • Nucleosynthesis and measurements of cosmic
    microwave background
  • ?h2100 10-5
  • To reach this limit, the effective viscosity has
    to be smaller than 2 106 Pa s.

33
Conclusions
  • Dilatonic waves can be searched for using
    superconducting gravimeters.
  • The sensitivity is currently limited by the
    uncertainty in the Earth model.
  • If the effective viscosity were determined to be
    smaller than 2 106 Pa s, this method would
    provide an upper limit better than the
    astrophysical limits.

34
Other possible future applications
  • Improved tests of the existence of a preference
    frame and an anisotropy of the gravitational
    constant.
  • Direct detection of gravitational waves using the
    Earth as the receiver.
  • Measurement of G
  • Tests for a distant dependence, time dependence
    and a spatial anisotropy.
  • Improved tests of the inverse square law.

J. M. Goodkind, Review of Scientific Instruments
70 (1999)
35
Summary
  • Superconducting gravimeters have been proved to
    be stable and sensitive in geophysical studies
    and also they have been used to study
    gravitational physics since 1970s.
  • The global network of superconducting gravimeters
    has been developed to study the Earths interior.
    By using the Earth as the test body, we
    investigate possible applications of the network
    to gravitational physics.
  • We have discussed the geophysical test of the
    universality of free-fall and the search for
    dilatonic waves.

36
Thank you.
  • Any new ideas for possible applications of SGs
    are welcome.
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