Abstract
We consider the minor process of (Hermitian) matrix diffusions with constant diagonal drifts. At any given time, this process is determinantal and we provide an explicit expression for its correlation kernel. This is a measure on the Gelfand–Tsetlin pattern that also appears in a generalization of Warren’s process (Electron. J. Probab. 12:573–590, 2007), in which Brownian motions have level-dependent drifts. Finally, we show that this process arises in a diffusion scaling limit from an interacting particle system in the anisotropic KPZ class in 2+1 dimensions introduced in Borodin and Ferrari (Commun. Math. Phys., 2008). Our results generalize the known results for the zero drift situation.
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Notes
For a set S, the notation \(\frac{1}{2\pi\mathrm{i}} \oint_{\varGamma_{S}}\mathrm{d}wf(w)\) means that the integral is taken over any positively oriented simple contour that encloses only the poles of f belonging to S.
Here, standard Brownian motions start from 0 and are normalized to have variance t at time t.
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Acknowledgements
The authors are grateful to M. Shkolnikov to point out how to use [18] to show Theorem 2 and to J. Warren for useful discussions. This work was supported by the German Research Foundation via the SFB 611–A12 and SFB 1060–B04 projects.
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Appendix: Determinantal Correlations
Appendix: Determinantal Correlations
Since we refer several times to Lemma 3.4 of [12], we report it here.
Lemma A.1
(Lemma 3.4 of [12])
Assume we have a signed measure on {\(x_{i}^{n},n=1,\ldots,N\), i=1,…,n} given in the form,
where \(x_{n+1}^{n}\) are some “virtual” variables and Z N is a normalization constant. If Z N ≠0, then the correlation functions are determinantal.
To write down the kernel we need to introduce some notations. Define
where \((a* b)(x,y)=\sum_{z\in\mathbb{Z}}a(x,z) b(z,y)\), and, for 1≤n<N,
Set \(\phi_{0}(x_{1}^{0},x)=1\). Then the functions
are linearly independent and generate the n-dimensional space V n . Define a set of functions \(\{\varPhi_{j}^{n}(x), j=0,\ldots,n-1\}\) spanning V n defined by the orthogonality relations
for 0≤i,j≤n−1.
Further, if \(\phi_{n}(x_{n+1}^{n},x)=c_{n} \varPhi_{0}^{(n+1)}(x)\), for some c n ≠0, n=1,…,N−1, then the kernel takes the simple form
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Ferrari, P.L., Frings, R. Perturbed GUE Minor Process and Warren’s Process with Drifts. J Stat Phys 154, 356–377 (2014). https://doi.org/10.1007/s10955-013-0887-5
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DOI: https://doi.org/10.1007/s10955-013-0887-5