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首页> 外文期刊>The Journal of Chemical Physics >The total neutron scattering cross section of solid methane in phase II
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The total neutron scattering cross section of solid methane in phase II

机译:第二阶段固体甲烷的总中子散射截面

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The total neutron scattering cross section per molecule sigma(tot) of solid methane in phase II was measured for incident neutron energies 0.5 meV less than or equal to E(n)less than or equal to 10 eV in the temperature range 0.3 K less than or equal to T less than or equal to 19.5 K. The sigma(tot) depends on the rotational, translational and vibrational dynamics of the CH4 molecule and shows significant dependence both on E-n and T. For E-n above 165 meV, which corresponds to the first vibrational excitation level of CH4, the sigma(tot) is equal to 4 sigma(p)(A/(A + 1))(2) = 80 b with proton mass A = I and a bound cross section sigma(p) = 80 b of a single proton. For E-n approximate to 6.5 meV, which is approximately the librational energy of the CH4 rotor, sigma(tot) approaches 205 b at all temperatures. This is the cross section of a rigid H-4 tetrahedron rotating freely about its fixed center; the effective mass is A = 4. For E-n < 6.5 meV, the interference effects of scattering from different protons within the same molecule, sensitive to nuclear spin symmetry, are observed. sigma(tot)similar to[I(1+1)](T) with total nuclear spin of the ortho, meta, para molecules I = 2, 1 or 0, respectively. For E-n-->0, two limiting cases can be distinguished. At high temperatures, the lower limit of sigma(tot) is given by the bound (incoherent) cross section of four protons 4 sigma(p) = 320 b. At low temperature, where only the ground state with I = 2 is occupied, sigma(tot) = 8 sigma(p) = 640 b. The experimental data compare well with a quantum-mechanical model and the mass-tenser approximation. Multiple rotational-translational-vibrational scattering contributions are discussed also. (C) 1998 American Institute of Physics. [S0021-9606(98)50632-0] [References: 55]
机译:在相变0.3 K以下的温度范围内,对于入射中子能量0.5 meV小于或等于E(n)小于或等于10 eV,测量相II中固体甲烷每分子sigma(tot)的总中子散射截面。等于或小于T等于或小于19.5K。sigma(tot)取决于CH4分子的旋转,平移和振动动力学,并且对En和T都显示出显着依赖性。对于大于165 meV的En,它对应于CH4的第一个振动激发能级,sigma(tot)等于4 sigma(p)(A /(A + 1))(2)= 80 b,质子质量A = I,束缚截面sigma(p) = 80 b的单个质子。对于大约6.5 meV的E-n(大约是CH4转子的自由能),在所有温度下sigma(tot)接近205b。这是刚性H-4四面体绕其固定中心自由旋转的横截面;有效质量为A =4。对于E-n <6.5 meV,观察到来自同一分子内不同质子的散射对核自旋对称性敏感的干扰效应。类似于[I(1 + 1)](T)的sigma(tot),分别具有邻,间,对位分子I = 2、1、0的总核自旋。对于E-n-> 0,可以区分两个极限情况。在高温下,sigma(tot)的下限由四个质子的结合(非相干)横截面4 sigma(p)= 320 b给出。在低温下,仅占据I = 2的基态,sigma(tot)= 8 sigma(p)= 640 b。实验数据与量子力学模型和质量张量近似进行了很好的比较。还讨论了多个旋转-平移-振动散射贡献。 (C)1998美国物理研究所。 [S0021-9606(98)50632-0] [参考:55]

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