lattice transformation 中文意思是什麼
lattice transformation
解釋
晶格轉變- lattice : n. 1. 格子。2. 【物理學】點陣；網路。3. 【建築】格構。vt. 1. 把…製成格子狀。2. 用格子覆蓋[裝飾]。
- transformation : n 轉變，變化；變形；【生物學】（尤指昆蟲的）轉化，變態，改造，改革；變質；【數學】變換；【電學】...
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We also discuss the statistical relations of the majorana lattice fermions and the majorana fermi fields respectively. chapter3 : new jordan - wigner - rype transformation between spin - 3 / 2 and fermions of two types is shown
第三章：介紹了在自旋- 3 2的自旋算符和雙費米子之間構建出的一種新的「 jordan - wigner 」類型的變換。 -
Then the structure unit of hexangular lattice is found according to the principle of invariable symmetry. renormalization transformation is processed when we regard the structure unit and the growth model as graphs before and after transformation respectively. after choosing the 11 thermodynamic function fugacity as parameter, we can write out the partition functions before and after transformation and the formula of renormalization transformation
然後根據對稱性不變的原則，從整體晶格中選取結構單元，把結構單元和生長模型分別作為重整化變換前、后的圖形來進行重整化變換，選取熱力學函數易逸度為參量，寫出了重整化變換前後的配分函數和重整化變換關系式，求出了這一變換的不動點。 -
Chapter2 : an important tool in studying one - dimensional spin lattice models is the kramers - wannier duality transformation
第二章：研究一維自旋格點模型的一個重要工具是「 kramers - wannier 」二重變換。 -
Based upon this transformation, we introduce another form of one - dimensional spin - 1 / 2 jordan - wigner transformation that maps the pauh spin operators onto the real majorana lattice fermions. next, its application in one - dimensional quantum ising spin chain model is displayed
基於該變換，我們介紹了另一種形式的一維自旋- 1 2的「 jordan - wigner 」交換，即用實的「 mbjorana 」格點費米子來描述泡利自旋算符。 -
After the coordinate transformation, the discrete velocity boltzmann equation is solved directly in computational domain to preserve the geometry of body. the results comparison of cylindrical couette flow at different size meshes, different lattice bgk models and different algorithms shows that, not only the precision of the incompressible lattice bgk model is satisfactory, but also the curvilinear coordinate algorithm is efficient
首先計算了存在理論解的圓柱couette流動，並針對不同數目的離散網格、不同格子模型以及不同坐標系演算法，對結果進行了比較，不僅再次印證了本文第四章給出的不可壓格子模型具有滿意的計算精度，而且表明本章的貼體坐標演算法是行之有效的。
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