例句與造句

1. One can transfer its action to diffeomprphsm invariant states.
2. By amenability there is an invariant state ? on " A ".
3. They also postulate the existence of a Poincar?invariant state called the vacuum and demand it is unique.
4. Another remarkable property of this invariant states that the Jones Polynomial of an alternating link is an alternating polynomial.
5. In this case, the loop invariant states what is known about the elements of the items examined so far  namely, that none of them matches the given item.
6. It's difficult to find invariant state in a sentence. 用invariant state造句挺難的
7. The Hamiltonian constraint maps diffeomorphism invariant states onto non-diffeomorphism invariant states as so does not preserve the diffeomorphism Hilbert space \ mathcal { H } _ { \ text { Diff } }.
8. The Hamiltonian constraint maps diffeomorphism invariant states onto non-diffeomorphism invariant states as so does not preserve the diffeomorphism Hilbert space \ mathcal { H } _ { \ text { Diff } }.
9. The aim of the loop representation, in the context of Yang-Mills theories is to avoid the redundancy introduced by Gauss gauge symmetries allowing to work directly in the space of Gauss gauge invariant states.
10. Thus, under time reversal, an invariant state must have vanishing EDM . In other words, a non-vanishing EDM signals both " P " and " T " symmetry-breaking.
11. For example, in the memory-invariant states there must be no cross-references ( or memory pointers ) between two SIPs; communication between SIPs occurs via higher-order communication channels managed by the operating system.
12. Therefore, for any given starting state, there are two possibilities : CPT leaves the state unchanged ( it's a CPT-invariant state ) or CPT switches back and forth between two states that are duals of each other.
13. However, there is no chance to define the Hamiltonian constraint operators corresponding to H ( x ) ( densely ) on \ mathcal { H } _ { Diff } because the Hamiltonian constraint operators do not preserve spatial diffeomorphism invariant states.
14. As mentioned above one cannot simply solve the spatial diffeomorphism constraint and then the Hamiltonian constraint, inducing a physical inner product from the spatial diffeomorphism inner product, because the Hamiltonian constraint maps spatially diffeomorphism invariant states onto non-spatial diffeomorphism invariant states.
15. As mentioned above one cannot simply solve the spatial diffeomorphism constraint and then the Hamiltonian constraint, inducing a physical inner product from the spatial diffeomorphism inner product, because the Hamiltonian constraint maps spatially diffeomorphism invariant states onto non-spatial diffeomorphism invariant states.
16. When one projects on \ Psi the position of the line does not matter because one is working on the space of diffeomorphism invariant states and so the line can be moved " closer " or " further " from the vertex without changing the result.
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