2012
DOI: 10.1007/s10955-012-0490-1
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Mayer and Virial Series at Low Temperature

Abstract: We analyze the Mayer and virial series (pressure as a function of the activity resp. the density) for a classical system of particles in continuous configuration space at low temperature. Particles interact via a finite range potential with an attractive tail. We propose physical interpretations of the Mayer and virial series' radii of convergence, valid independently of the question of phase transition: the Mayer radius corresponds to a fast increase from very small to finite density, and the virial radius co… Show more

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Cited by 17 publications
(11 citation statements)
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References 19 publications
(54 reference statements)
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“…When p = p β → 0 slower than any exponential, it is still true that g(β) → e 0 0 . When βp β = exp(−βν) with ν > 0, one can show with [26,27] At pressures vanishing faster than exp(−β|e 0 0 |), the most likely configurations have very large spacings (dilute gas phase, (β) → ∞) and the previous results no longer apply. For lim inf 1 β log(βp β ) > e 0 0 , we expect that large deviations principles with rate functions E 0 bulk and E 0 surf − min E 0 surf still hold (in fact our proofs still show weak large deviations principles).…”
Section: Small Positive Temperaturementioning
confidence: 93%
“…When p = p β → 0 slower than any exponential, it is still true that g(β) → e 0 0 . When βp β = exp(−βν) with ν > 0, one can show with [26,27] At pressures vanishing faster than exp(−β|e 0 0 |), the most likely configurations have very large spacings (dilute gas phase, (β) → ∞) and the previous results no longer apply. For lim inf 1 β log(βp β ) > e 0 0 , we expect that large deviations principles with rate functions E 0 bulk and E 0 surf − min E 0 surf still hold (in fact our proofs still show weak large deviations principles).…”
Section: Small Positive Temperaturementioning
confidence: 93%
“…Recent works [59,131,133] investigate the exponentially small region of convergence of the Mayer series close to T = ρ = 0, where things can be proved in any dimension. Namely, they considered the limit T → 0 and ρ → 0 with the constraint that T log ρ → ν (recall that ρ ∼ z = e µ/T at small activity, so this is similar to fixing µ).…”
Section: Extensionsmentioning
confidence: 99%
“…It is the smoothing effect of this term that gets lost in that approximation, and possibly a lot of new kinks appear in this way. We know that these additional kinks correspond to cross-overs inside the gas phase, but not to sharp phase transitions (see [8] for a discussion of this). Hence, the full ideal mixture captures the behaviour of the physical system much better than the function studied in [9].…”
Section: Discussionmentioning
confidence: 99%