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New version: FiniteMPS v1.6.0 #122224

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### Breaking changes
- Rewrite `addIntr!` and `addObs!` and change the interface. For example, consider a hopping term, now the usage becomes
```julia
addIntr!(Root, (Fdag, F), (i, j), (true, true), strength; Z = Z)
```
where `(true, true)` means both operators are fermionic.  Similarly, 
```julia
addObs!(Tree, (Fdag, F), (i, j), (true, true); Z = Z)
```
for the calculation of single-particle correlations. 
- Now a multi-site correlation with duplicated site indices can automatically reduce to a shorter term. For example, in the case of $U_1 \times SU_2$ symmetry, the pairing correlation $\langle \Delta_{12}^\dagger \Delta_{23}\rangle$ can be simply calculated via 
```julia
addObs!(Tree, U1SUFermions.ΔₛdagΔₛ, (1, 2, 2, 3), (true, true, true, true); Z = U1SUFermions.Z)
```
- Support adding 3-site terms, e.g. chiral operator $S_i \cdot (S_j \times S_k)$ pinning field, to the Hamiltonian.

UUID: 6b572690-f317-4dad-a5fe-5fe73a0b7d42
Repo: https://github.com/Qiaoyi-Li/FiniteMPS.jl.git
Tree: 05fc60737c2886785f89296ac73ad4071998cbf7

Registrator tree SHA: 17aec322677d9b81cdd6b9b9236b09a3f1374c6a
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@JuliaTagBot JuliaTagBot merged commit 10476ae into master Dec 31, 2024
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@JuliaTagBot JuliaTagBot deleted the registrator-finitemps-6b572690-v1.6.0-63d53449fe branch December 31, 2024 20:02
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