To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure no-reply@cambridge.org
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
We study Bose gases in $d \ge 2$ dimensions with short-range repulsive pair interactions at positive temperature, in the canonical ensemble and in the thermodynamic limit. We assume the presence of hard Poissonian obstacles and focus on the non-percolation regime. For sufficiently strong interparticle interactions, we show that almost surely there cannot be Bose–Einstein condensation into a sufficiently localized, normalized one-particle state. The results apply to the canonical eigenstates of the underlying one-particle Hamiltonian.
We present several formulations of the large deviation principle for empirical measures in the V topology, depending on the initial distribution. The case V = B(S) is further studied.
We relate the rate functions introduced in Chapters 2 and 3 to the functions I and Isubindex ψ. We establish conditions for the equality I= Isubindex ψ. We introduce the conditions V.1′–V.4.
We obtain lower bounds for bounded vector-valued additive functionals and use them to obtain lower bounds for empirical measures. We prove a lower semicontinuity property of Λ.
We study large deviations for general vector-valued additive functionals. The relationship between large deviations for empirical measures and large deviations for additive functionals is discussed.