{"id":703,"date":"2019-03-29T11:14:53","date_gmt":"2019-03-29T11:14:53","guid":{"rendered":"https:\/\/blog.vanabel.cn\/?p=703"},"modified":"2019-03-29T11:14:53","modified_gmt":"2019-03-29T11:14:53","slug":"alpha-diaoheyingzhaoliudechubianzhiwentizhicunzaixing","status":"publish","type":"post","link":"https:\/\/blog.vanabel.cn\/?p=703","title":{"rendered":"$\\alpha$-\u8c03\u548c\u6620\u7167\u6d41\u7684\u521d\u8fb9\u503c\u95ee\u9898\u4e4b\u5b58\u5728\u6027"},"content":{"rendered":"<p>\u6211\u4eec\u9996\u5148\u6765\u770b$\\alpha$\u8c03\u548c\u6620\u7167\u6d41, \u5176\u65b9\u7a0b\u53ef\u4ee5\u5199\u4f5c<br \/>\n$$\\left\\{\\begin{aligned}<br \/>\n  \\partial_t u^\\beta-\\Delta u^\\beta-(\\alpha-1) \\frac{u_{kl}^{\\beta\\gamma}u_k^\\gamma u_l^\\beta}{1+\\lvert \\nabla u \\rvert^2}&#038;=\\Gamma^\\beta(u)(\\nabla u,\\nabla u),\\quad x\\in M;\\\\<br \/>\n  u(\\cdot,0)&#038;=u_0\\in C^\\infty(M), \\quad x\\in M;\\\\<br \/>\n  u^n(x,t)&#038;=0, \\quad (x,t)\\in\\partial M\\times[0,T];\\\\<br \/>\n  \\frac{\\partial u^\\beta}{\\partial\\nu}&#038;=0,\\quad (x,t)\\in \\partial M\\times [0,T],\\quad \\beta=1,2,\\ldots, n-1.<br \/>\n\\end{aligned}\\right.$$<br \/>\n\u6211\u4eec\u5c06\u8003\u8651\u5176\u7ebf\u6027\u5f62\u5f0f, \u5373<br \/>\n$$<br \/>\n  \\partial_t u^\\beta-\\Delta u^\\beta-(\\alpha-1) \\frac{u_{kl}^{\\beta\\gamma}w_k^\\gamma w_l^\\beta}{1+\\lvert \\nabla w \\rvert^2}=\\Gamma^\\beta(w)(\\nabla w,\\nabla w),\\quad x\\in M.<br \/>\n$$<br \/>\n\u6539\u5199\u6210\u6807\u51c6\u7684\u5f62\u5f0f<br \/>\n$$<br \/>\n  \\mathcal{L}u=f,<br \/>\n$$<!--more--><\/p>\n<p>\u5373<br \/>\n$$<br \/>\nl_{\\beta\\gamma}u^\\gamma_{kl}=f_\\beta(x,t),<br \/>\n$$<br \/>\n\u5176\u4e2d<br \/>\n$$<br \/>\nl_{\\beta\\gamma}(x,t,\\partial_x,\\partial_t)=\\delta_{\\beta\\gamma}\\partial_t-\\left( \\delta_{kl}\\delta_{\\beta\\gamma}+(\\alpha-1) \\frac{w_k^\\gamma w_l^\\beta}{1+\\lvert \\nabla w \\rvert^2} \\right)\\partial_k\\partial_l,<br \/>\n$$<br \/>\n\u4ee5\u53ca<br \/>\n$$<br \/>\nf_\\beta(x,t)=\\Gamma^\\beta(w)(\\nabla w,\\nabla w).<br \/>\n$$<br \/>\n\u8fd9\u4e9b\u7cfb\u6570\u6ee1\u8db3[<a href='#Solonnikov1965boundary'>N\/A<\/a>,p. 8]\u7684\u6761\u4ef6, \u5373<\/p>\n<p>1.<br \/>\n$$\\begin{aligned}<br \/>\n  l_{\\beta\\gamma}(x,t,i\\xi\\lambda,p\\lambda^2)&#038;=\\delta_{\\beta\\gamma}p\\lambda^2-\\left( \\delta_{kl}\\delta_{\\beta\\gamma}+(\\alpha-1)\\frac{w_k^\\gamma w_l^\\beta}{1+\\lvert \\nabla w \\rvert^2} \\right)(i\\xi^k\\lambda)(i\\xi^l\\lambda)\\\\<br \/>\n                                             &#038;=\\left( \\delta_{\\beta\\gamma}p+\\delta_{\\beta\\gamma}\\lvert \\xi \\rvert^2+(\\alpha-1)\\frac{w_k^\\gamma w_l^\\beta \\xi^k\\xi^l}{1+\\lvert \\nabla w \\rvert^2} \\right)\\lambda^2<br \/>\n                                             :=l_{\\beta\\gamma}^0(x,t,i\\xi,p)\\lambda^2.<br \/>\n\\end{aligned}$$<br \/>\n\u5176\u4e2d, \u4ee5$l_{\\beta\\gamma}^0$\u4f5c\u4e3a\u7cfb\u6570\u7684\u7b97\u5b50$\\mathcal{L}_0$\u79f0\u4e3a\u539f\u7b97\u5b50$\\mathcal{L}$\u7684\u4e3b\u90e8. \u5728\u6211\u4eec\u7684\u60c5\u5f62\u7531\u4e8e\u6ca1\u6709\u4f4e\u9636\u5bfc\u6570\u9879, $l_{\\beta\\gamma}^0=l_{\\beta\\gamma}$.<\/p>\n<p>2. \u629b\u7269\u6027\u6761\u4ef6. \u5373\u4ee5$l_{\\beta\\gamma}^0(x,t,i\\xi, p)$\u4e3a$(\\beta,\\gamma)$\u5143\u7d20\u7684\u77e9\u9635$L_0$\u7684\u884c\u5217\u5f0f\u4f5c\u4e3a$p$\u7684\u591a\u5f62\u5f0f\u4e4b\u6839$p_s$\u6ee1\u8db3<br \/>\n$$<br \/>\n\\mathrm{Re}p_s\\leq-\\delta \\lvert \\xi \\rvert^2,\\quad \\delta>0.<br \/>\n$$<\/p>\n<p>\u4e8b\u5b9e\u4e0a, \u82e5\u4ee4<br \/>\n$$<br \/>\nX=\\sqrt{\\alpha-1}\\frac{\\xi\\cdot\\nabla w}{\\sqrt{1+\\lvert \\nabla w \\rvert^2}},<br \/>\n$$<br \/>\n\u5219<br \/>\n$$<br \/>\nL(x,t,i\\xi,p)=\\det L_0(x,t,i\\xi,p)=\\left\\lvert (p+\\lvert \\xi \\rvert^2)E +XX^T \\right\\rvert,<br \/>\n$$<br \/>\n\u5176\u7279\u5f81\u6839\u4e3a<br \/>\n$$<br \/>\np_1=-\\lvert \\xi \\rvert^2-(\\alpha-1)\\frac{\\xi^kw_k^\\gamma \\xi^lw_l^\\gamma}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\np_2=p_3=\\cdots=p_n=-\\lvert \\xi \\rvert^2.<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230<br \/>\n$$<br \/>\n  \\frac{\\xi^kw_k^\\gamma \\xi^lw_l^\\gamma}{1+\\lvert \\nabla w \\rvert^2}<br \/>\n  \\leq \\lvert \\xi \\rvert^2.<br \/>\n$$<br \/>\n\u53ef\u89c1, \u6211\u4eec\u53ef\u53d6$\\delta=1$.<\/p>\n<p>3. \u8fb9\u754c\u6761\u4ef6. \u5728$\\Gamma=\\partial\\Omega\\times(0,T)$\u4e0a, \u6211\u4eec\u7684\u4e00\u822c\u8fb9\u754c\u6761\u4ef6\u662f<br \/>\n$$<br \/>\n  \\mathcal{B}u=\\Phi,<br \/>\n$$<br \/>\n\u5373<br \/>\n$$<br \/>\n\\sum_{\\beta=1}^n B_{q\\beta}(x,t,\\partial_x,\\partial_t)u^\\beta(x,t)=\\Phi_q(x,t),\\quad q=1,2,\\ldots, br,<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230\u5bf9\u6211\u4eec\u7684\u60c5\u5f62, $b=1$, $r=n$, \u5176\u4e2d$2b$\u5c31\u662f\u629b\u7269\u65b9\u7a0b\u7684\u9636, \u800c$r$\u5c31\u662f$\\det L_0$\u4f5c\u4e3a$p$\u7684\u591a\u5f62\u5f0f\u7684\u6700\u9ad8\u6b21\u5e42. \u6839\u636e\u6211\u4eec\u7684\u8fb9\u503c\u6761\u4ef6, \u6211\u4eec\u77e5\u9053<br \/>\n$$<br \/>\n(B_{q\\beta}(x,t,\\partial_x,\\partial_t))_{n\\times n}=\\left(<br \/>\n  \\begin{array}{cccc}<br \/>\n    \\sum_{k=1}^m\\nu^k\\partial_k&#038;0&#038;\\cdots &#038;0\\\\<br \/>\n    0&#038;\\sum_{k=1}^m\\nu^k\\partial_k&#038;\\cdots &#038;0\\\\<br \/>\n    \\vdots&#038;\\vdots&#038;\\cdots&#038;\\vdots\\\\<br \/>\n    0 &#038;0 &#038;\\sum_{k=1}^m\\nu^k\\partial_k&#038;0\\\\<br \/>\n    0 &#038;0 &#038;0 &#038;1 \\\\<br \/>\n\\end{array}<br \/>\n\\right),<br \/>\n$$<br \/>\n\u5176\u4e2d,<br \/>\n$$<br \/>\n\\nu=(\\nu^1,\\ldots, \\nu^m),\\quad m=\\dim M,<br \/>\n$$<br \/>\n\u662f$\\partial\\Omega\\times\\left\\{ t \\right\\}$\u5728$(x,t)$\u5904\u7684\u5185\u6cd5\u5411. \u7279\u522b\u5730,<br \/>\n$$<br \/>\nB_{q\\beta}(x,t,i\\xi\\lambda,p\\lambda^{2b})=\\left\\{<br \/>\n  \\begin{array}{cl}<br \/>\n    i\\sum_{k=1}^m\\nu^k \\xi^k\\lambda,&#038;q=\\beta=1,2,\\ldots, n-1,\\\\<br \/>\n    1,&#038;q=\\beta=n,\\\\<br \/>\n    0,&#038;\\text{otherwise}.<br \/>\n  \\end{array}<br \/>\n  \\right.<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230$B_{q\\beta}$\u90fd\u662f\u9f50\u6b21\u591a\u5f62\u5f0f, \u6545\u5176\u4e3b\u90e8\u6070\u597d\u7b49\u4e8e\u81ea\u8eab, \u5373$B_{q\\beta}^0=B_{q\\beta}$. <\/p>\n<p>4. \u4e92\u8865\u6761\u4ef6(complementary condition). <\/p>\n<ul>\n<li>\u5bf9\u8fb9\u754c\u6761\u4ef6, \u6211\u4eec\u7684\u4e92\u8865\u6761\u4ef6\u5982\u4e0b: \u5047\u8bbe$\\mathrm{Re}p\\geq -\\delta_1\\lvert \\zeta \\rvert^2$, \u5176\u4e2d$0<\\delta_1<\\delta$\u4e14$\\lvert p \\rvert^2+\\lvert \\zeta \\rvert^4>0$, \u6ce8\u610f\u8fd9\u91cc$p$\u4e3a\u590d\u6570. \u5219\u53ef\u4ee5\u8bc1\u660e<\/li>\n<\/ul>\n<p>$$<br \/>\nL(x,t,i(\\zeta+\\tau\\nu),p)<br \/>\n$$<br \/>\n\u4f5c\u4e3a$\\tau$\u7684\u51fd\u6570\u6709$n$\u4e2a\u865a\u90e8\u4e3a\u6b63\u7684\u6839$\\tau_s^+$, \u4ee5\u53ca\u865a\u90e8\u4e3a\u8d1f\u7684\u6839$\\tau_s^-$, \u5176\u4e2d$\\zeta=\\zeta(x)$\u662f$x\\in\\partial\\Omega$\u5904\u7684\u5207\u5411\u91cf, \u800c$\\nu=\\nu(x)$\u4e3a$x\\in\\partial\\Omega$\u5904\u7684\u5355\u4f4d\u5185\u6cd5\u5411\u91cf.<\/p>\n<p>\u4e8b\u5b9e\u4e0a, \u5728\u6211\u4eec\u7684\u60c5\u5f62, \u76f4\u63a5\u9a8c\u8bc1\u77e5<br \/>\n$$<br \/>\nL(x,t,i(\\zeta+\\tau\\nu),p)=0<br \/>\n$$<br \/>\n\u7684\u6839\u5206\u522b\u4e3a<br \/>\n$$\\begin{aligned}<br \/>\n  \\tau^\\pm_2&#038;=\\cdots=\\tau^\\pm_n=\\pm i\\sqrt{p+\\lvert \\zeta \\rvert^2},\\\\<br \/>\n  \\tau^\\pm_1&#038;=\\frac{\\frac{2(\\alpha-1)\\nabla_\\nu w\\cdot\\nabla_\\zeta w}{1+\\lvert \\nabla w \\rvert^2}\\pm\\sqrt{\\left( \\frac{2(\\alpha-1)(\\nabla_\\nu w\\cdot\\nabla_\\zeta w)}{1+\\lvert \\nabla w \\rvert^2} \\right)^2-4\\left( 1+\\frac{(\\alpha-1)\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)\\left( p+\\lvert \\zeta \\rvert^2+\\frac{(\\alpha-1)\\lvert \\nabla_\\zeta w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)}}{2\\left( 1+\\frac{(\\alpha-1)\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)}\\\\<br \/>\n            &#038;=\\pm i\\sqrt{p+\\lvert \\zeta \\rvert^2}+o(\\alpha-1).<br \/>\n\\end{aligned}$$<br \/>\n\u5bf92-\u503c\u51fd\u6570$\\sqrt{p+\\lvert \\zeta \\rvert^2}$\u6211\u4eec\u53ef\u4ee5\u9009\u53d6\u5176\u4e2d\u4e00\u4e2a\u5206\u652f, \u4f7f\u5f97\u5176\u5b9e\u90e8\u662f\u5927\u4e8e\u96f6\u7684. \u4e3a\u65b9\u4fbf\u8d77\u89c1, \u6211\u4eec\u4ee4$\\tau_0=i\\sqrt{p+\\lvert \\zeta \\rvert^2}$.<\/p>\n<p>\u73b0\u5728, \u6211\u4eec\u4ee4<br \/>\n$$<br \/>\nL_0^+(\\zeta,\\tau,p)=(\\tau-\\tau_1^+)\\cdots(\\tau-\\tau_n^+)=(\\tau-\\tau_1^+)(\\tau-\\tau_0)^{n-1},<br \/>\n$$<br \/>\n\u4ee5\u53ca<br \/>\n$$<br \/>\nR(\\zeta,\\tau,p)=B_0(i\\zeta,i\\tau,p)\\hat L_0(i\\zeta,i\\tau,p),<br \/>\n$$<br \/>\n\u5176\u4e2d<br \/>\n$$<br \/>\nB_0(i\\zeta,i\\tau,p)=B_0(x_0,t_0,i(\\zeta+\\tau\\nu),p)=\\mathrm{diag}(\\tau,\\cdots,\\tau,1)_{n\\times n},\\quad (x_0,t_0)\\in\\partial\\Omega\\times(0,T),<br \/>\n$$<br \/>\n\u800c<br \/>\n$$<br \/>\nL_0(i\\zeta,i\\tau,p)=L_0(x_0,t_0,i(\\zeta+\\tau\\nu),p)=(p+\\lvert \\zeta \\rvert^2+\\tau^2)E+X_\\tau^TX_\\tau,<br \/>\n$$<br \/>\n\u5176\u4e2d<br \/>\n$$<br \/>\nX_\\tau=\\sqrt{\\frac{\\alpha-1}{1+\\lvert \\nabla w \\rvert^2}} (\\nabla_\\zeta w+\\tau\\nabla_\\nu w).<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230$E+X_\\tau^TX_\\tau$\u7684\u4f34\u968f\u77e9\u9635<br \/>\n$$<br \/>\n(E+X_\\tau^TX_\\tau)^*=(1+X_\\tau X_\\tau^T)E-X_\\tau^TX_\\tau.<br \/>\n$$<br \/>\n\u6216\u8005<br \/>\n$$<br \/>\n(\\lambda E+X_\\tau^TX_\\tau)^*=(\\lambda^{n-1}+\\lambda^{n-2} X_\\tau X_\\tau^T)E-\\lambda^{n-2} X_\\tau^TX_\\tau.<br \/>\n$$<br \/>\n\u56e0\u6b64<br \/>\n$$<br \/>\n\\hat L_0(i\\zeta,i\\tau,p)=\\left( (p+\\lvert \\zeta \\rvert^2+\\tau^2)^{n-1}+(p+\\lvert \\zeta \\rvert^2+\\tau^2)^{n-2}X_\\tau X_\\tau^T \\right)E<br \/>\n-(p+\\lvert \\zeta \\rvert^2+\\tau^2)^{n-2}X_\\tau^T X_\\tau.<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230<br \/>\n$$<br \/>\n\\begin{aligned}<br \/>\n  X_\\tau X_\\tau^T&#038;=\\lvert X_\\tau \\rvert^2=(\\alpha-1)\\frac{\\lvert \\nabla_\\zeta w+\\tau \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2}\\\\<br \/>\n                 &#038;=(\\alpha-1)\\frac{1}{1+\\lvert \\nabla w \\rvert^2}\\left( \\tau^2\\lvert \\nabla_\\nu w \\rvert^2+2\\tau\\nabla_\\zeta w\\nabla_\\nu w+\\lvert \\nabla_\\nu w \\rvert^2 \\right).<br \/>\n\\end{aligned}<br \/>\n$$<\/p>\n<p>\u6211\u4eec\u9996\u5148\u5bf9$n=2$\u6765\u8fdb\u884c\u9a8c\u8bc1. \u6b64\u65f6<br \/>\n$$<br \/>\nL_0^+(i\\zeta,i\\tau,p)=(\\tau-\\tau_0)(\\tau-\\tau_1^+),<br \/>\n$$<br \/>\n\u800c<br \/>\n$$<br \/>\nB_0(i\\zeta,i\\tau,p)=\\mathrm{diag}(\\tau,1),<br \/>\n$$<br \/>\n\u4ee5\u53ca<br \/>\n$$<br \/>\n\\begin{aligned}<br \/>\n  \\hat L_0(i\\zeta,i\\tau,p)&#038;=\\left( p+\\lvert \\zeta \\rvert^2+\\tau^2+(\\alpha-1)\\frac{\\tau^2\\lvert \\nabla_\\nu w \\rvert^2+2\\tau\\nabla_\\zeta w\\nabla_\\nu w^T+\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)E\\\\<br \/>\n                          &#038;\\qquad-(\\alpha-1)\\frac{\\tau^2\\nabla_\\nu w^T\\nabla_\\nu w+2\\tau\\nabla_\\nu w^T\\nabla_\\zeta w+\\nabla_\\zeta w^T\\nabla_\\zeta w}{1+\\lvert \\nabla w \\rvert^2}.<br \/>\n\\end{aligned}$$<br \/>\n\u56e0\u6b64\u82e5\u8bb0<br \/>\n$$<br \/>\nR(i\\zeta,i\\tau,p) :=B_0(i\\zeta,i\\tau,p)\\hat L_0(i\\zeta,i\\tau,p),<br \/>\n$$<br \/>\n\u5219<br \/>\n$$<br \/>\n\\begin{aligned}<br \/>\n  R_{11}&#038;=\\tau\\left( p+\\lvert \\zeta \\rvert^2+\\tau^2+(\\alpha-1)\\frac{\\tau^2\\lvert \\nabla_\\nu w \\rvert^2+2\\tau\\nabla_\\zeta w\\nabla_\\nu w^T+\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)\\\\<br \/>\n        &#038;\\qquad-(\\alpha-1)\\tau\\frac{\\tau^2\\nabla_\\nu w^1\\nabla_\\nu w^1+2\\tau\\nabla_\\nu w^1\\nabla_\\zeta w^1+\\nabla_\\zeta w^1\\nabla_\\zeta w^1}{1+\\lvert \\nabla w \\rvert^2}\\\\<br \/>\n  R_{12}&#038;=-(\\alpha-1)\\tau \\frac{\\tau^2\\nabla_\\nu w^1\\nabla_\\nu w^2+2\\tau\\nabla_\\nu w^1\\nabla_\\zeta w^2+\\nabla_\\zeta w^1\\nabla_\\zeta w^2}{1+\\lvert \\nabla w \\rvert^2}\\\\<br \/>\n  R_{21}&#038;=-(\\alpha-1)\\frac{\\tau^2\\nabla_\\nu w^2\\nabla_\\nu w^1+2\\tau\\nabla_\\nu w^2\\nabla_\\zeta w^1+\\nabla_\\zeta w^2\\nabla_\\zeta w^1}{1+\\lvert \\nabla w \\rvert^2}\\\\<br \/>\n  R_{22}&#038;=\\left( p+\\lvert \\zeta \\rvert^2+\\tau^2+(\\alpha-1)\\frac{\\tau^2\\lvert \\nabla_\\nu w \\rvert^2+2\\tau\\nabla_\\zeta w\\nabla_\\nu w^T+\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2} \\right)\\\\<br \/>\n        &#038;\\qquad-(\\alpha-1)\\frac{\\tau^2\\nabla_\\nu w^2\\nabla_\\nu w^2+2\\tau\\nabla_\\nu w^2\\nabla_\\zeta w^2+\\nabla_\\zeta w^2\\nabla_\\zeta w^2}{1+\\lvert \\nabla w \\rvert^2}.<br \/>\n\\end{aligned}<br \/>\n$$<br \/>\n\u6ce8\u610f\u5230<br \/>\n$$<br \/>\np+\\lvert \\zeta \\rvert^2+\\tau_1^{+2}+(\\alpha-1)\\frac{\\lvert \\nabla_{\\zeta+{\\tau_1^+}\\nu}w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2}=0,<br \/>\n$$<br \/>\n\u56e0\u6b64<br \/>\n$$<br \/>\n\\begin{aligned}<br \/>\n  &#038;p+\\lvert \\zeta \\rvert^2+\\tau^2+(\\alpha-1)\\frac{\\tau^2\\lvert \\nabla_\\nu w \\rvert^2+2\\tau\\nabla_\\zeta w\\nabla_\\nu w^T+\\lvert \\nabla_\\nu w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2}\\\\<br \/>\n  &#038;\\qquad=\\tau^2-\\tau_1^{+2}+(\\alpha-1)\\frac{(\\tau^2-\\tau_1^{+2})\\lvert \\nabla_\\nu w \\rvert^2+2(\\tau-\\tau_1^+)\\nabla_\\zeta w\\nabla_\\nu w^T}{1+\\lvert \\nabla w \\rvert^2}.<br \/>\n\\end{aligned}<br \/>\n$$<br \/>\n\u4ee4<br \/>\n$$\\begin{aligned}<br \/>\n  a&#038;=(\\alpha-1)\\frac{|\\nabla_\\nu w|^2}{1+\\lvert \\nabla w \\rvert^2},\\\\<br \/>\n  a_{11}&#038;=(\\alpha-1)\\frac{|\\nabla_\\nu w^1|^2}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  a_{12}=a_{21}=(\\alpha-1)\\frac{\\nabla_\\nu w^1\\nabla_\\nu w^2}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  a_{22}=(\\alpha-1)\\frac{|\\nabla_\\nu w^2|^2}{1+\\lvert \\nabla w \\rvert^2},\\\\<br \/>\n  b&#038;=(\\alpha-1)\\frac{\\nabla_\\nu w\\nabla_\\zeta w^T}{1+\\lvert \\nabla w \\rvert^2},\\\\<br \/>\n  b_{11}&#038;=(\\alpha-1)\\frac{\\nabla_\\nu w^1\\nabla_\\zeta w^1}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  b_{12}=(\\alpha-1)\\frac{\\nabla_\\nu w^1\\nabla_\\zeta w^2}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  b_{21}=(\\alpha-1)\\frac{\\nabla_\\nu w^2\\nabla_\\zeta w^1}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  b_{22}=(\\alpha-1)\\frac{\\nabla_\\nu w^2\\nabla_\\zeta w^2}{1+\\lvert \\nabla w \\rvert^2},\\\\<br \/>\n  c&#038;=(\\alpha-1)\\frac{\\lvert \\nabla_\\zeta w \\rvert^2}{1+\\lvert \\nabla w \\rvert^2},\\\\<br \/>\n  c_{11}&#038;=(\\alpha-1)\\frac{\\lvert \\nabla_\\zeta w^1 \\rvert^2}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  c_{12}=c_{21}=(\\alpha-1)\\frac{ \\nabla_\\zeta w^1\\nabla_\\zeta w^2}{1+\\lvert \\nabla w \\rvert^2},\\quad<br \/>\n  c_{22}=(\\alpha-1)\\frac{\\lvert \\nabla_\\zeta w^2 \\rvert^2}{1+\\lvert \\nabla w \\rvert^2},<br \/>\n  \\end{aligned}$$<br \/>\n  \u5219<br \/>\n  $$\\begin{aligned}<br \/>\n    R_{11}&#038;=\\tau \\left( (\\tau^2-\\tau_1^{+2})(1+a)+2(\\tau-\\tau_1^+)b \\right)-a_{11}\\tau^3-2b_{11}\\tau^2-c_{11}\\tau,\\\\<br \/>\n    R_{12}&#038;=-a_{12}\\tau^3-2b_{12}\\tau^2-c_{12}\\tau,\\\\<br \/>\n    R_{21}&#038;=-a_{21}\\tau^2-2b_{21}\\tau-c_{21},\\\\<br \/>\n    R_{22}&#038;=\\left( (\\tau^2-\\tau_1^{+2})(1+a)+2(\\tau-\\tau_1^+)b \\right)-a_{22}\\tau^2-2b_{22}\\tau-c_{22}.<br \/>\n  \\end{aligned}$$<br \/>\n  \u56e0\u6b64, \u6a21\u6389$L_0^+=(\\tau-\\tau_1^+)(\\tau-\\tau_0)$, \u6211\u4eec\u5f97\u5230<br \/>\n  $$<br \/>\n    \\begin{aligned}<br \/>\n      R_{11}&#8217;&#038;=\\tau\\left(\\tau_0^2(1+a-a_{11})+\\tau_0\\tau_1^+(1+a-a_{11})-a_{11}\\tau_1^{+2}-2b_{11}(\\tau_0+\\tau_1^+)+2b\\tau_0-c_{11}\\right)\\\\<br \/>\n             &#038;\\qquad-\\tau_0\\tau_1^+\\left( (1+a-a_{11})(\\tau_0+\\tau_1^+)-2b_{11}+2b \\right),\\\\<br \/>\n      R_{12}&#8217;&#038;=-\\tau\\left( a_{12}(\\tau_0^2+\\tau_0\\tau_1^++\\tau_1^+)+2b_{12}(\\tau_0+\\tau_1^+)+c_{12} \\right)\\\\<br \/>\n            &#038;\\qquad-\\tau_0\\tau_1^+\\left( a_{12}(\\tau_0+\\tau_1^+)+2b_{12} \\right),\\\\<br \/>\n      R_{21}&#8217;&#038;=-\\tau\\left( a_{12}(\\tau_0+\\tau_1^+)+2b_{21} \\right)\\\\<br \/>\n             &#038;\\qquad+a_{12}\\tau_0\\tau_1^+-c_{12},\\\\<br \/>\n      R_{22}&#8217;&#038;=\\tau\\left( (1+a-a_{22})(\\tau_0+\\tau_1^+)-2b_{22}+2b \\right)\\\\<br \/>\n             &#038;\\qquad-\\tau_1^+\\left( (1+a)\\tau_1^++(1+a-a_{22})\\tau_0^++2b \\right)-c_{22}.<br \/>\n    \\end{aligned}<br \/>\n  $$<br \/>\n  \u6211\u4eec\u7684\u8fb9\u754c\u4e92\u8865\u6761\u4ef6\u8981\u6c42<br \/>\n  $$<br \/>\n    \\mathrm{rank}R&#8217;=2.<br \/>\n  $$<br \/>\n  \u8fd9\u5728$\\alpha=1$\u7684\u60c5\u5f62, \u53ea\u9700\u8981$\\tau_0\\neq0$\u5373\u53ef.<\/p>\n<ul>\n<li>\u5bf9\u521d\u503c\u6761\u4ef6, \u6211\u4eec\u7684\u4e92\u8865\u6761\u4ef6\u5982\u4e0b: \u6ce8\u610f\u5230, \u6211\u4eec\u7684\u521d\u503c\u6761\u4ef6\u6539\u5199\u6210\u4e00\u822c\u5f62\u5f0f\u4e3a<\/li>\n<\/ul>\n<p>$$<br \/>\n  \\mathcal{C}u|_{t=0}=\\Psi,<br \/>\n$$<br \/>\n\u5373<br \/>\n$$<br \/>\n\\sum_{\\beta=1}^n C_{q\\beta}(x,\\partial_x,\\partial_t)u^\\beta|_{t=0}=\\psi_q(x), \\quad q=1,2,\\ldots,n.<br \/>\n$$<br \/>\n\u5728\u6211\u4eec\u7684\u60c5\u5f62, $C_{q\\beta}=\\delta_{q\\beta}$, \u56e0\u6b64\u521d\u503c\u7b97\u5b50$\\mathcal{C}$\u7684\u4e3b\u90e8$\\mathcal{C}^0=\\mathcal{C}$. \u5982\u679c\u6211\u4eec\u8bb0\u4ee5$C^0_{q\\beta}=\\delta_{q\\beta}$\u4e3a\u5143\u7d20\u7684\u77e9\u9635\u4e3a$C^0$, \u5219<br \/>\n$$<br \/>\nC^0(x,i\\xi,p)=E_n.<br \/>\n$$<\/p>\n<p>\u56de\u5fc6, $L_0$\u4e3a$l_{\\beta\\gamma}^0(x,t,i\\xi,p)$\u4f5c\u4e3a$(\\beta,\\gamma)$\u5143\u7d20\u7684\u77e9\u9635. \u5728\u6211\u4eec\u7684\u60c5\u5f62,<br \/>\n$$<br \/>\nL_0(x,0,0,p)=(\\delta_{\\beta\\gamma}p)_{n\\times n}=p E_n.<br \/>\n$$<br \/>\n\u82e5\u8bb0$\\hat L_0(x,t,i\\xi,p)$\u4e3a$L_0(x,t,i\\xi,p)$\u7684\u4f34\u968f\u77e9\u9635\u4e3a$C^0$,<br \/>\n\u5219\u5728\u6211\u4eec\u7684\u60c5\u5f62<br \/>\n$$<br \/>\n\\hat L_0(x,0,0,p)=p^{n-1}E_n.<br \/>\n$$<br \/>\n\u800c\u6240\u8c13\u7684\u521d\u503c\u6761\u4ef6\u7684\u4e92\u8865\u6027\u6761\u4ef6\u5373\u662f\u8bf4\u77e9\u9635<br \/>\n$$<br \/>\nC_0(x,0,p)\\hat L_0(x,0,0,p)=p^{n-1}E_n<br \/>\n$$<br \/>\n\u7684\u884c\u5411\u91cf\u6a21\u6389\u9996\u9879\u7cfb\u6570\u4e3a1\u7684\u591a\u5f62\u5f0f(\u5373$\\det L_0(x,0,0,0)$\u7684\u6700\u9ad8\u6b21\u9879)$p^n$\u662f\u7ebf\u6027\u65e0\u5173\u7684.<\/p>\n<div class='bibtex'>\n\t<div class='bibtex_h'>\u53c2\u8003\u6587\u732e<\/div>\n\t<ol><\/ol><\/div>","protected":false},"excerpt":{"rendered":"<p>\u6211\u4eec\u9996\u5148\u6765\u770b$\\alpha$\u8c03\u548c\u6620\u7167\u6d41, \u5176\u65b9\u7a0b\u53ef\u4ee5\u5199\u4f5c $$\\left\\{\\begin{aligned} \\&hellip; <a class=\"more-link\" href=\"https:\/\/blog.vanabel.cn\/?p=703\">\u7ee7\u7eed\u9605\u8bfb<span class=\"screen-reader-text\">$\\alpha$-\u8c03\u548c\u6620\u7167\u6d41\u7684\u521d\u8fb9\u503c\u95ee\u9898\u4e4b\u5b58\u5728\u6027<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[2],"tags":[139,140,31],"class_list":["post-703","post","type-post","status-publish","format-standard","hentry","category-math","tag-alpha-diaoheyingzhao","tag-hubutiaojian","tag-31","entry"],"_links":{"self":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/703","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=703"}],"version-history":[{"count":2,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/703\/revisions"}],"predecessor-version":[{"id":705,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/703\/revisions\/705"}],"wp:attachment":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=703"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=703"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=703"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}