Differences

This shows you the differences between two versions of the page.

--- documentation:ref:diractrace [2015/11/20 19:11]
poslavskysv [Description]
+++ documentation:ref:diractrace [2015/11/21 12:33] (current)
@@ Line 3: / Line 3: @@
 ====Description====
   * ''%%DiracTrace%%'' calculates trace of Dirac matrices in $D$ dimensions
@@ Line 9: / Line 10: @@
   * One can directly set trace of identity matrix (e.g. for dimensional regularisation): ''%%DiracTrace[[Dimension: D, TraceOfOne: 4]]%%''
-  * By default ''DiracTrace'' uses notation ''G_m'' for $\gamma_m$, ''G5'' for $\gamma_5$ and ''e_abcd'' for Levi-Civita tensor. %%DiracTrace[G, G5, eps]%%'' or ''%%DiracTrace[[Gamma: G, Gamma5: G5, LeviCivita: eps]]%%'' specifies the notation for $\gamma_m$, $\gamma_5$ and Levi-Civita tensor.
+  * By default ''DiracTrace'' uses notation ''G_m'' for $\gamma_m$, ''G5'' for $\gamma_5$ and ''e_abcd'' for Levi-Civita tensor.  ''%%DiracTrace[G, G5, eps]%%'' or ''%%DiracTrace[[Gamma: G, Gamma5: G5, LeviCivita: eps]]%%'' specifies the notation for $\gamma_m$, $\gamma_5$ and Levi-Civita tensor.
   * ''%%DiracTrace[[Simplifications: rules]]%%'' will apply additional simplification ''rules'' to each processed trace
 ====Examples====
 ----
@@ Line 17: / Line 20: @@
 <sxh groovy; gutter: false>
 defineMatrices 'G_a', 'G5', Matrix1.matrix
-println DiracTrace['G_a'] >> 'Tr[G_a*G_b]'.t
+println DiracTrace >> 'Tr[G_a*G_b]'.t
 </sxh>
 <sxh plain; gutter: false>
@@ Line 27: / Line 30: @@
 //set up matrix objects
 defineMatrices 'G_a', 'G5', Matrix1.matrix
-//DiracTrace transformation
-def dTrace = DiracTrace[[Gamma: 'G_a']]
 //calculate trace
-println  dTrace >> 'Tr[(p_a*G^a + m)*G_m*(q_a*G^a-m)*G_n]'.t
+println  DiracTrace >> 'Tr[(p_a*G^a + m)*G_m*(q_a*G^a-m)*G_n]'.t
 </sxh>
 <sxh plain; gutter: false>
@@ Line 41: / Line 42: @@
 //set up matrix objects
 defineMatrices 'G_a', 'G5', Matrix1.matrix
-//DiracTrace transformation
-def dTrace = DiracTrace[[Gamma: 'G_a', Gamma5: 'G5', LeviCivita: 'e_abcd']]
 //calculate trace
-println dTrace >> 'Tr[G_a*G_b*G_c*G_d*G5]'.t
+println DiracTrace >> 'Tr[G_a*G_b*G_c*G_d*G5]'.t
 </sxh>
 <sxh plain; gutter: false>
@@ Line 50: / Line 49: @@
 </sxh>
 <sxh groovy; gutter: true; first-line: 7>
-println dTrace >> 'Tr[(p_a*G^a + m)*G_m*G5*(q_a*G^a-m)*G_n]'.t
+println DiracTrace >> 'Tr[(p_a*G^a + m)*G_m*G5*(q_a*G^a-m)*G_n]'.t
 </sxh>
 <sxh plain; gutter: false>
@@ Line 107: / Line 106: @@
 ----
-''DiracTrace'' expands out products of sums containing traces of $\gamma$-matrices and leaves unexpanded other parts of expressions:
+Use another notation for gamma matrices:
 <sxh groovy; gutter: false>
-defineMatrices 'G_a', 'G5', Matrix1.matrix
+defineMatrices 'F_\\mu', 'F5', Matrix2.matrix
-def expr = '(k_c+p_c)*(k_d+p_d) + Tr[(p^a + k^a)*(p^b + k^b)*G_a*G_b*G_c*G_d]'.t
+def dTrace = DiracTrace[[Gamma: 'F_\\mu', Gamma5: 'F5', LeviCivita: 'Eps_{\\mu\\nu\\alpha\\beta}']]
-println dTrace >> expr
+println dTrace >> 'Tr[F_\\mu*F_\\nu*F_\\alpha*F_\\beta * F5]'.t
 </sxh>
 <sxh plain; gutter: false>
-   > (k_c+p_c)*(k_d+p_d)+4*g_cd*p_b*p^b+4*k_b*k^b*g_cd+8*k^b*g_cd*p_b
+   > -4*I*Eps_{\mu\nu\alpha\beta}
 </sxh>
 ====Options====
+  * ''Simplifications'': one can specify additional simplifications that will be applied to each evaluated trace:<sxh groovy; gutter: false>
+defineMatrices 'G_a', 'G5', Matrix1.matrix
+def expr = 'Tr[(p^a + k^a)*(p^b + k^b)*G_a*G_b*G_c*G_d]'.t
+def mandelstam = setMandelstam([k_a: '0', p_a: '0', q_a: 'm', r_a: 'm'], 's', 't', 'u')
+println DiracTrace[[Simplifications: mandelstam]] >> expr
+</sxh><sxh plain; gutter: false>
+   > 4*s*g_{cd}
+</sxh>which is same as<sxh groovy; gutter: false>
+println( (DiracTrace & mandelstam) >> expr )
+</sxh><sxh plain; gutter: false>
+   > 4*s*g_{cd}
+</sxh>
+  * ''ExpandAndEliminate'': ''DiracTrace'' expands out products of sums containing traces of $\gamma$-matrices using [[ExpandAndEliminate]] transformation. One can replace it with another instance using ''%%DiractTrace[[ExpandAndEliminate: tr]]%%''.
+  * ''LeviCivitaSimplify'': When traces involve $\gamma_5$, ''DiracTrace'' uses [[LeviCivitaSimplify]] in for simplifying resulting expressions with Levi-Civita tensors. One can replace the default instance of [[LeviCivitaSimplify]] with another one using ''%%DiractTrace[[ExpandAndEliminate: tr]]%%''.
 ====See also====
   * Related guides: [[documentation:guide:applying_and_manipulating_transformations]], [[documentation:guide:Setting up matrix objects]], [[documentation:guide:list_of_transformations]]
   * Related tutorials: [[documentation:tutorials:Compton scattering in QED]]
-  * Related transformations: [[documentation:ref:LeviCivitaSimplify]], [[documentation:ref:UnitaryTrace]]
+  * Related transformations: [[documentation:ref:DiracSimplify]], [[documentation:ref:DiracOrder]],  [[documentation:ref:LeviCivitaSimplify]], [[documentation:ref:UnitaryTrace]]
-  * JavaDocs: [[http://api.redberry.cc/redberry/1.1.8/java-api//cc/redberry/physics/feyncalc/DiracTraceTransformation.html| DiracTraceTransformation]]
+  * JavaDocs: [[http://api.redberry.cc/redberry/1.1.9/java-api//cc/redberry/physics/feyncalc/DiracTraceTransformation.html| DiracTraceTransformation]]
   * Source code: [[https://bitbucket.org/redberry/redberry/src/tip/physics/src/main/java/cc/redberry/physics/feyncalc/DiracTraceTransformation.java|DiracTraceTransformation.java]]