{
	"cells" : 
	[
		
		{
			"cell_origin" : "client",
			"cell_type" : "latex",
			"cells" : 
			[
				
				{
					"cell_origin" : "client",
					"cell_type" : "latex_view",
					"source" : "\\algorithm{expand_diracbar}{Simplify the Dirac bar of a composite object.}\n\nRewrite the Dirac conjugate of a product of spinors and gamma matrices\nas a product of Dirac and hermitean conjugates. This uses\n\\begin{equation} \n\\bar\\psi = i \\psi^\\dagger\\Gamma^0\\,,\n\\end{equation}\ntogether with \n\\begin{equation}\n\\Gamma_m^{\\dagger} = \\Gamma_0\\Gamma_m\\Gamma_0 \\,.\n\\end{equation}\nFor example,"
				}
			],
			"hidden" : true,
			"source" : "\\algorithm{expand_diracbar}{Simplify the Dirac bar of a composite object.}\n\nRewrite the Dirac conjugate of a product of spinors and gamma matrices\nas a product of Dirac and hermitean conjugates. This uses\n\\begin{equation} \n\\bar\\psi = i \\psi^\\dagger\\Gamma^0\\,,\n\\end{equation}\ntogether with \n\\begin{equation}\n\\Gamma_m^{\\dagger} = \\Gamma_0\\Gamma_m\\Gamma_0 \\,.\n\\end{equation}\nFor example,"
		},
		
		{
			"cell_origin" : "client",
			"cell_type" : "input",
			"cells" : 
			[
				
				{
					"cell_origin" : "server",
					"cell_type" : "latex_view",
					"source" : "\\begin{dmath*}{}\\bar{\\Gamma^{m n p} \\psi}\\end{dmath*}"
				}
			],
			"source" : "\\bar{#}::DiracBar.\n\\psi::Spinor(dimension=10).\n\\Gamma{#}::GammaMatrix.\nex:=\\bar{\\Gamma^{m n p} \\psi};"
		},
		
		{
			"cell_origin" : "client",
			"cell_type" : "input",
			"cells" : 
			[
				
				{
					"cell_origin" : "server",
					"cell_type" : "latex_view",
					"source" : "\\begin{dmath*}{}\\bar{\\psi} \\Gamma^{m n p}\\end{dmath*}"
				}
			],
			"source" : "expand_diracbar(_);"
		},
		
		{
			"cell_origin" : "client",
			"cell_type" : "input",
			"source" : ""
		}
	],
	"description" : "Cadabra JSON notebook format",
	"version" : 1.0
}