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  2. 26 Feb 2018: 23. Figure 24: Reconstruction of vertices by the DBSCAN clustering algorithm (with =0.16875mm and minPoints = 2) PminT = 3GeV, σ = 0.1mm. ... 24. Figure 26: Reconstruction of vertices by the merge clustering algorithm (with mergedistance set to 0.525mm,
  3. Multiparticle instability in a spin-imbalanced Fermi gas

    www.tcm.phy.cam.ac.uk/~tmw38/Whitehead18.pdf
    8 Jan 2018: The effect of Pauli blocking has been carefully analyzed[22–24] for the product of two (N,N) = (1,1) instabilities,and found to give only a small correction to the ... B81, 174514 (2010). [23] W. V. Pogosov and M. Combescot, Physica C 471, 566
  4. Stability of fractional Chern insulators in the effective continuum…

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.97.035159.pdf
    5 Feb 2018: 3045. 00.410.811.2. xy. g(r. ). (b) (c). 0 12 24 36 012. ... 2436. 00.51. 11.5. 0 12 24 36 012. 2436. 00.51. 11.5.
  5. 20 Mar 2018: Eb =1. Nb. RBb. EL(R) (24). 3.2. ImplementationThe following VQMC calculations are carried out us-. ... Beryllium 4 -14.32830 -14.66735 [7]Boron 5 -23.42837 -24.65393 [8]. The calculated variational energies (EV ) of a succession of atomicsystems.
  6. Parameterizing Unresolved Mesoscale Motions in Atmospheric Dispersion …

    www.tcm.phy.cam.ac.uk/~tmw38/jamc-d-17-0075.1.pdf
    15 May 2018: 1976) proposed parameterizations of wind variability. over a range of time periods up to 24 h,.
  7. 26 Feb 2018: 24). We see that the term proportional to σ̂↠corresponds. to exiting both the qubit and the cavity.

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