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Christian Corda INFN-VIRGO Scalar gravitational waves from Scalar-Tensor Gravity: production and response of interferometers Miniworkshop "Supersymmetry, Supergravity, Superstrings" March 19-21 2007 Aula 131 - Dipartimento di Fisica - Largo B.Pontecorvo,3 - Pisa

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Christian Corda INFN-VIRGO

Scalar gravitational wavesfrom Scalar-Tensor Gravity:production and response of

interferometers Miniworkshop

"Supersymmetry, Supergravity, Superstrings"March 19-21 2007

Aula 131 - Dipartimento di Fisica - Largo B.Pontecorvo,3 - Pisa

Introduction1) Mechanism of production of SGW from Scalar-

Tensor Gravity2) Massless case: invariance of the signal in three

different gauges3) Massless case: the frequency-dependent angular

pattern4) The small massive caseGeneralized previous results analyzed in the low-

frequencies approximation

Mechanism of production of SGWfrom Scalar-Tensor Gravity

Most general action for STG in literature

Considering the transformation

previous action reads

BD-like theory

Field equations

Klein-Gordon

Linearized theory in vacuum

Minkowski background + minimum for W

We assume

obteining

with

Effective BD

The massless case

Most simple case:

Gauge transforms (Lorenz condition)

Solutions are plan waves

Purely scalar wave: line element

TT gauge extended to scalar waves

The response of aninterferometer

Literature: low-frequencies approximation

Method of “bouncing photon” : the variationof space-time due to the scalar field iscomputed in all the travel of the photon

Computation of the variation of proper timein presence of the SGW

In the Fourier domain

The “Shibata, Nakao and Nakamura” gaugefor SGW

Purely scalar wave: line element

Reanalyzed

Same results of the TT gauge

In the Fourier domain

Used a time transform

The local Lorentz gauge for SGW:three different effects

The motion of test masses

The travel of photons in curved spacetime

The shifting of time

Gauge invariance recovered

In the Fourier domain

Angular pattern for SGW

Line element in u direction

variation of proper timein presence of the SGW inu direction

Response function in u direction

Same analysis: responsefunction in v direction

Total frequency-dependent responsefunction

Agrees with

Low frequencies

The small massive case

Treating scalars like classical waves

Frequencies have to fall in

Interval for the mass

Known for string-dilaton gravity

Parameterization of the field with the phase-velocityPresence of the mass: third component ofRiemann

Previous analysis in the local Lorentz gaugegeneralized with the aid of Fourier theorems,two effects

The motion of test masses

The travel of photons in curved spacetime

Total frequency-dependent longitudinalresponse function

ConclusionsRealistic possibility to detect SGW indifferent gauges

Realistic possibility to detect a longitudinalcomponentThe investigation of scalar components ofGW could be a tool to discriminateamong several theories of gravity

Next papersCorda C. The “Shibata, Nakao and Nakamuragauge for SGW” submitted to GRG gr-qc0610157Corda C. “The importance of the magneticcomponents of gravitational waves in theresponse function of interferometersgr-qc 0702080 accepted for IJMPD

Capozziello S.,Corda C. and de Laurentis MF“On the correct frame for theories: Jordan frameversus Einstein frame”