2007
DOI: 10.1086/520917
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The Cepheid Phase Lag Revisited

Abstract: We compute the phase lags between the radial velocity curves and the light curves $\Delta \Phi_1= \phi^{V_r}_1 - \phi^{mag}_1$ for classical Cepheid model sequences both in the linear and the nonlinear regimes. The nonlinear phase lags generally fall below the linear ones except for high period models where they lie above, and of course for low pulsation amplitudes where the two merge. The calculated phase lags show good agreement with the available observational data of normal amplitude Galactic Cepheids. The… Show more

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Cited by 33 publications
(49 citation statements)
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“…Turner et al (2006b) also doubt that V1726 Cyg pulsates in the first overtone: its carefully determined luminosity is consistent with that of a fundamental mode pulsator. The existence of fundamental mode Cepheids pulsating with small amplitude is also predicted by theoretical computations (Szabó et al 2007).…”
Section: Resultssupporting
confidence: 54%
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“…Turner et al (2006b) also doubt that V1726 Cyg pulsates in the first overtone: its carefully determined luminosity is consistent with that of a fundamental mode pulsator. The existence of fundamental mode Cepheids pulsating with small amplitude is also predicted by theoretical computations (Szabó et al 2007).…”
Section: Resultssupporting
confidence: 54%
“…Theoretical calculations modelling the pulsation of Cepheids have been unable to fully reproduce the P-A diagram delineated by observational data. Model calculations by Szabó et al (2007), however, confirm theoretically that the spread in photometric amplitude at a given pulsation period is partly caused by differences in the location of the datapoints within the instability strip (see their Fig. 7).…”
Section: Introductionmentioning
confidence: 77%
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“…One objective of these calculations must be to explain the origin of the phase lag of +0.15 cycles between maximum light and minimum radius in V652 Her. Phase lags exist in Cepheids but in the opposite sense (-0.25 cycles) and are understood in terms of linear (non-adiabatic) effects associated with the thin hydrogen ionization zone moving through mass layers almost as a discontinuity (Castor 1968;Szabó et al 2007). Since the hydrogen and first helium ionization zones play no role in V652 Her (too little hydrogen and too hot), it is suggested that an interaction between the second helium ionization zone and the nickel/iron opacity bump at 2 × 10 5 K will be important.…”
Section: Discussionmentioning
confidence: 99%