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1.
设(Mr,T)是一个在r维闭光滑流形上的不平凡光滑对合,可证对合的不动点集是P(1,n)×HP(1),n为奇数,则(Mr,T)协边于零.  相似文献   

2.
设(Mr,T)是一个在r维光滑闭流形M上的不平凡光滑对合,它的不动点集为F.本文给出了F=m1∪i=1 RRi(4n)∪m2∪i=1HPi(n)(4n<r)时对合的协边类,其中RP(4n),HP(n)分别表示4n维实射影空间和n维四元数射影空间.  相似文献   

3.
不动点集为F=U_(i=1)~mRP_i(1)×HP_i(n)的对合   总被引:1,自引:0,他引:1  
李向红  吕桂稳  侯铎 《数学学报》2006,49(2):265-270
(M,T)是一个在r维光滑闭流形M上的不平凡光滑对合,它的不动点集为F.本文给出了F=U(i=1)~m RPi(1)×HPi(n)时对合的协边类,其中HP(n)表示n维四元数射影空间.  相似文献   

4.
设(M~(4n k 2),T)是一个带有光滑对合T的光滑闭流形,T的不动点集为RP(4)■ P(4,2n-1).本文决定了(M~(4n k 2),T)的所有协边类.  相似文献   

5.
设(M,T)是一个带有光滑对合T的光滑闭流形,T的不动点集为RP(8)P(8,2n-1).本文证明了(M,T)必协边于(RP(8)×RP(8),twist)和(P(8,RP(2n)),T′)之一.  相似文献   

6.
设(M,T)是一个带有光滑对合T的光滑闭流形,T的不动点集为RP(8)() P(8,2n-1).本文证明了(M,T)必协边于(RP(8)×RP(8),twist)和(P(8,RP(2n)),T')之一.  相似文献   

7.
陈德华 《数学研究》2005,38(2):148-156
设(M,T)是一个光滑闭流形上的对合,不动点集为F=RP(4)UP(4,2n-1),则它的每一个对合(M,T)必协边(RP(4)×RP(4),twist)和(P(4,2n),T')之一.  相似文献   

8.
刘秀贵 《数学年刊A辑》2002,23(6):779-788
本文证明了具有光滑对合T的(4n+2m+3+κ)-维闭流形,如果对合的不动点集为F=P(2m+1,2n+1),其中2m+2n=2+22+...+2b(2b为2n二幂展开式的最大二幂),m=4a或m=4a+3(a为非负整数),0<κ≠2,则对合T协边于零.  相似文献   

9.
研究具有光滑对合T的4n 2m 2 K维闭流形M,如果对合的不动点集是F=P(2m,2n 1),其中m是4的倍数,证明了当n≥m>0时,(M,T)协边于零;当m>n≥0时,且m-n为偶数时,(M,T)协边于零.  相似文献   

10.
不动点集为RP(2)∪L~1(p)的对合   总被引:2,自引:2,他引:0  
(M3+ k,T)是在光滑闭流形上的一个非平凡光滑对合 ,它的不动点集为 RP(2 )∪ L 1 (p ) .本文给出了带对合的流形 (M3+ k,T)的协边类  相似文献   

11.
Let (M^2m+4n+k-2, T) be a smooth closed manifold with a smooth involution T whose fixed point set is RP(2^m) ∪ P(2^m, 2n - 1) (m 〉 3, n 〉 0). For 2n ≥ 2^m, (M^2m+4n+k-2, T) is bordant to (P(2^m, RP(2n)), To).  相似文献   

12.
本文的主要建立非齐性度量测度空间上双线性强奇异积分算子$\widetilde{T}$及交换子$\widetilde{T}_{b_{1},b_{2}}$在广义Morrey空间$M^{u}_{p}(\mu)$上的有界性. 在假设Lebesgue可测函数$u, u_{1}, u_{2}\in\mathbb{W}_{\tau}$, $u_{1}u_{2}=u$,且$\tau\in(0,2)$. 证明了算子$\widetilde{T}$是从乘积空间$M^{u_{1}}_{p_{1}}(\mu)\times M^{u_{2}}_{p_{2}}(\mu)$到空间$M^{u}_{p}(\mu)$有界的, 也是从乘积空间$M^{u_{1}}_{p_{1}}(\mu)\times M^{u_{2}}_{p_{2}}(\mu)$到广义弱Morrey空间$WM^{u}_{p}(\mu)$有界的,其中$\frac{1}{p}=\frac{1}{p_{1}}+\frac{1}{p_{2}}$及$1相似文献   

13.
The author investigated how big the lag increments of a 2-parameter Wiener process is in [1]. In this paper the limit inferior results for the lag increments are discussed and the same results as the Wiener process are obtained. For example, if $\[\mathop {\lim }\limits_{T \to \infty } \{ \log T/{a_T} + \log (\log {b_T}/a_T^{1/2} + 1)\} /\log \log T = r,0 \leqslant r \leqslant \infty \] $ then $\[\mathop {\lim }\limits_{\overline {T \to \infty } } \mathop {\sup }\limits_{{a_T} \leqslant t \leqslant T} \mathop {\sup }\limits_{t \leqslant s \leqslant T} \mathop {\sup }\limits_{R \in L_s^*(t)} |W(R)|/d(T,t) = {\alpha _r},a.s.,\] $ $\[\mathop {\lim }\limits_{\overline {T \to \infty } } \mathop {\sup }\limits_{{a_T} \leqslant t \leqslant T} \mathop {\sup }\limits_{R \in {{\tilde L}_T}(t)} |W(R)|/d(T,t) = {\alpha _r},a.s.,\] $ where $\alpha _r=(r/(r+1))^{1/2}$, $L*_s(t)$ and $\tider L_T(t)$ are the sets of rectangles which satisfy some conditions. Moreover, the limit inferior results of another class of lag increments are discussed.  相似文献   

14.
Let A be a standard operator algebra on a Banach space of dimension 〉 1 and B be an arbitrary algebra over Q the field of rational numbers. Suppose that M : A → B and M^* : B → A are surjective maps such that {M(r(aM^*(x)+M^*(x)a))=r(M(a)x+xM(a)), M^*(r(M(a)x+xM(a)))=r(aM^*(x)+M^*(x)a) for all a ∈ A, x ∈ B, where r is a fixed nonzero rational number. Then both M and M^* are additive.  相似文献   

15.
On an almost quaternionic manifold we study the integrability of almost complex structures which are compatible with the almost quaternionic structure . If , we prove that the existence of two compatible complex structures forces to be quaternionic. If , that is is an oriented conformal 4-manifold, we prove a maximum principle for the angle function of two compatible complex structures and deduce an application to anti-self-dual manifolds. By considering the special class of Oproiu connections we prove the existence of a well defined almost complex structure on the twistor space of an almost quaternionic manifold and show that is a complex structure if and only if is quaternionic. This is a natural generalization of the Penrose twistor constructions.

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16.
In this paper, we initiate the oscillation theory for $h$-fractional difference equations of the form \begin{equation*} \begin{cases} _{a}\Delta^{\alpha}_{h}x(t)+r(t)x(t)=e(t)+f(t,x(t)),\ \ \ t\in\mathbb{T}_{h}^{a},\ \ 1<\alpha<2,\x(a)=c_{0},\ \ \Delta_{h}x(a)=c_{1},\ \ \ c_{0}, c_{1}\in\mathbb{R}, \end{cases} \end{equation*} where $_{a}\Delta^{\alpha}_{h}$ is the Riemann-Liouville $h$-fractional difference of order $\alpha,$ $\mathbb{T}_{h}^{a}:=\{a+kh, k\in\mathbb{Z^{+}}\cup\{0\}\},$ and $a\geqslant0,$ $h>0.$ We study the oscillation of $h$-fractional difference equations with Riemann-Liouville derivative, and obtain some sufficient conditions for oscillation of every solution. Finally, we give an example to illustrate our main results.  相似文献   

17.
李玉成  兰文华 《数学学报》2008,51(5):959-964
令H~∞(D)表示单位圆盘D上的有界解析函数全体构成的代数,对于■∈H~∞(D),在某种条件下,证明T=M■是一个指标为n的Cowen-Douglaus算子,并且给出了■(T)/rad■(T)可交换的一个充分条件.当n=1时,刻画了T的换位.  相似文献   

18.
Let be a symmetric Finsler manifold, endowed with the Busemann volume form, and let be its unit disk bundle endowed with the canonical symplectic volume form. It is shown that , where is the volume of the unit disk in . Moreover, equality holds if and only if is Riemannian.

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19.
We provide two regularity criteria for the weak solutions of the 3D micropolar fluid equations, the first one in terms of one directional derivative of the velocity, i.e., $\partial_{3}u$, while the second one is is in terms of the behavior of the direction of the velocity $\frac{u}{|u|}$. More precisely, we prove that if \begin{equation*} \partial_{3}u \in L^{\beta}(0,T;L^{\alpha}(\mathbb{R}^{3}))\quad\text{ with }\frac{2}{\beta}+\frac{3}{\alpha}\leq 1+\frac{1}{\alpha}, 2&lt; \alpha \leq\infty, 2\leq\beta&lt; \infty; \end{equation*} or \begin{equation*} \operatorname{div}\left(\frac{u}{|u|}\right)\in L^{\frac{4}{1-2r}}(0,T;\dot{X}_{r}(\mathbb{R}^{3}))\quad \text{ with } 0\leq r&lt; \frac{1}{2}, \end{equation*} then the weak solution $(u(x,t),\omega(x,t))$ is regular on $\mathbb{R}^{3}\times [0,T]$. Here $\dot{X}_{r}(\mathbb{R}^{3})$ is the multiplier space.  相似文献   

20.
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