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| Main Authors: | , , |
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| Format: | Preprint |
| Published: |
2023
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| Subjects: | |
| Online Access: | https://arxiv.org/abs/2310.11686 |
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| _version_ | 1866916268280381440 |
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| author | Li, Xin Zhang, Liping Ke, Yifen |
| author_facet | Li, Xin Zhang, Liping Ke, Yifen |
| contents | In this paper, a classical deflation process raised by Dayton, Li and Zeng is realized for the Brent equations, which provides new bounds for local dimensions of the solution set. Originally, this deflation process focuses on isolated solutions. We generalize it to the case of irreducible components and a related conjecture is given. We analyze its realization and apply it to the Brent equations. The decrease of the nullities is easily observed. So the deflation process can be served as a useful tool for determining the local dimensions. In addition, our result implies that along with the decrease of the tensor rank, the singular solutions will become more and more. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2310_11686 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Deflation conjecture and local dimensions of Brent equations Li, Xin Zhang, Liping Ke, Yifen Algebraic Geometry In this paper, a classical deflation process raised by Dayton, Li and Zeng is realized for the Brent equations, which provides new bounds for local dimensions of the solution set. Originally, this deflation process focuses on isolated solutions. We generalize it to the case of irreducible components and a related conjecture is given. We analyze its realization and apply it to the Brent equations. The decrease of the nullities is easily observed. So the deflation process can be served as a useful tool for determining the local dimensions. In addition, our result implies that along with the decrease of the tensor rank, the singular solutions will become more and more. |
| title | Deflation conjecture and local dimensions of Brent equations |
| topic | Algebraic Geometry |
| url | https://arxiv.org/abs/2310.11686 |