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31.
Frame-spun knots are constructed by spinning a knot of lower dimension about a framed submanifold of . We show that all frame-spun knots are slice (null-cobordant).

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32.
A -frame is a lattice in which countable joins exist and binary meets distribute over countable joins. In this paper, the category MFrm, of metric -frames, is introduced, and it is shown to be equivalent to the category MLFrm u, of metric Lindelöf frames.Finally, it is shown that the complete metric -frames are exactly the cozero parts of complete metric Lindelöf frames.  相似文献   
33.
When a cardinal B-spline of order greater than 1 is used as the scaling function to generate a multiresolution approximation of L 2=L 2(R) with dilation integer factor M2, the standard matrix extension approach for constructing compactly supported tight frames has the limitation that at least one of the tight frame generators does not annihilate any polynomial except the constant. The notion of vanishing moment recovery (VMR) was introduced in our earlier work (and independently by Daubechies et al.) for dilation M=2 to increase the order of vanishing moments. This present paper extends the tight frame results in the above mentioned papers from dilation M=2 to arbitrary integer M2 for any compactly supported M-dilation scaling functions. It is shown, in particular, that M compactly supported tight frame generators suffice, but not M–1 in general. A complete characterization of the M-dilation polynomial symbol is derived for the existence of M–1 such frame generators. Linear spline examples are given for M=3,4 to demonstrate our constructive approach.  相似文献   
34.
Inhomogeneous multidimensional cosmological models with a higher-dimensional space-time manifold 0 i=1 n Mi (n 1) are in stigated under dimensional reduction to a D 0-dimensional effective non-minimally coupled -model which generalizes the familiar Brans–Dicke model. The general form of the Einstein frame representation of multidimensional solutions known in the Brans–Dicke frame is given with respect to cosmic synchronous time. As an example, the transformation is demonstrated explicitly for the generalized Kasner solutions where it is shown that solutions in the Einstein frame show no inflation of the external space although they can undergo deflation after the cosmic synchronous time inversion.  相似文献   
35.
H. Cao  Y. Wu  H. Zhou 《组合设计杂志》2008,16(5):351-363
A modified (k, λ)‐frame of type gu is a modified (k, λ)‐GDD whose blocks can be partitioned into holey parallel classes, each of which is with respect to some group. Modified frames can be used to construct some other resolvable designs such as resolvable group divisible designs and semiframes. In this article, we shall investigate the existence of modified frames with block size 3. © 2007 Wiley Periodicals, Inc. J Combin Designs 16: 351–363, 2008  相似文献   
36.
We obtain a condition implying that the union of two frame sequences is also a frame sequence. Christensen found a condition for this in terms of orthogonal projections. We phrase our condition by use of the angle between closed subspaces. Also a lower bound formula is obtained. We then apply the results to find conditions for a frame containing a Riesz basis to be a Riesz frame.  相似文献   
37.
本文研究了带有Radon-Nikodym导数的算子值自由Fisher信息量.利用模框架理论,得到了一个半圆元和一个子代数之间的合并自由关系,推广了D.Voiculescu等人的工作.  相似文献   
38.
程俊芳  李登峰 《数学学报》2008,51(5):877-888
设E=■或■,■(x)∈L~2(R~2)且■_(jk)(x)=2■(E~jx-k),其中j∈Z,k∈Z~2.若{■_(jk)|jJ∈Z,k∈Z~2}构成L~2(R~2)的紧框架,则称■(x)为E-紧框架小波.本文给出E-紧框架小波是MRA E-紧框架小波的一个充要条件,即E紧框架小波■来自多尺度分析当且仅当线性空间F_■(ξ)的维数为0或1,其中F_■(ξ)=■(ξ)|j■1},■_j(ξ)={■((E~T)~j(ξ+2kπ))}_(k∈EZ~2,j■1。  相似文献   
39.
Abstact: In this article, we present a new construction to obtain uniform frames with block size four and index one. The known existence results for (4, 1)‐frames and (4, 3)‐frames are both improved with a small number of possible exceptions. © 2000 John Wiley & Sons, Inc. J Combin Designs 9: 28–39, 2001  相似文献   
40.
孪生子佯谬   总被引:1,自引:0,他引:1  
邢杰  赵长春  郝会颖 《物理与工程》2005,15(4):14-15,52
本文从一个新的角度来阐释孪生子佯谬的症结所在,详细分析了由于双胞胎兄弟所在参考系的不对称性导致的荒谬结论,并在两个惯性系下分别做了计算,最后的结论是相同的,并不存在矛盾,同时印证了所有的惯性系是平权的这一大前提!  相似文献   
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