Effects of Flavor Dependence on Weak Decays of <svg     style="vertical-align:-4.698pt;width:34.262501px;" id="M1" height="21.737499" version="1.1" viewBox="0 0 34.262501 21.737499" width="34.262501"  xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,15.825)"><path id="x1D43D" d="M434 650l-5 -28q-60 -8 -75 -20.5t-25 -69.5l-71 -395q-20 -107 -57.5 -168t-106.5 -94q-40 -18 -61 -20l-10 32q77 23 113 108q21 50 41 160l68 377q10 57 -1.5 69.5t-76.5 20.5l6 28h261z" /></g><g transform="matrix(.022,-0,0,-.022,10.307,15.825)"><path id="x2F" d="M368 703l-264 -866h-60l265 866h59z" /></g><g transform="matrix(.022,-0,0,-.022,19.542,15.825)"><path id="x1D713" d="M642 419q-50 -36 -71 -94q-28 -78 -68 -170q-39 -89 -114 -135q-34 -21 -83 -31l-45 -219l-31 -31q-8 7 -15 29.5t-2 45.5l35 172q-153 10 -153 169q0 28 6 84q7 68 7 88q0 48 -27 48q-18 0 -51 -28l-7 26q62 75 118 75q49 0 49 -90q0 -47 -5 -81q-10 -72 -10 -108
q0 -117 82 -133l87 455l62 19l7 -2l-99 -478q91 12 131 120q34 93 51 154q20 73 36 88q42 40 103 56z" /></g>

		
	
</svg> and <svg     style="vertical-align:-0.0pt;width:14.8125px;" id="M2" height="15.025" version="1.1" viewBox="0 0 14.8125 15.025" width="14.8125"  xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,14.975)"><path id="x3A5" d="M648 625l-6 -15q-6 1 -13 1q-42 0 -86.5 -30.5t-81.5 -88.5q-93 -143 -93 -298v-72q0 -60 15.5 -75.5t84.5 -19.5v-27h-284v27q67 4 83 19.5t16 75.5v78q0 163 -53 273q-64 136 -186 136q-18 0 -38 -3l-5 26q62 33 122 33q114 0 173 -150q33 -79 44 -206h5q21 106 59 180
q33 76 84.5 126t108.5 50q30 0 51 -40z" /></g>

		
	
</svg>

<table>Variation of average transverse quark momentum with respect to physical meson masses.</table>

Advances in High Energy Physics

fig1

Figure 1

Figure 1: Effects of Flavor Dependence on Weak Decays of <svg     style="vertical-align:-4.698pt;width:34.262501px;" id="M1" height="21.737499" version="1.1" viewBox="0 0 34.262501 21.737499" width="34.262501"  xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,15.825)"><path id="x1D43D" d="M434 650l-5 -28q-60 -8 -75 -20.5t-25 -69.5l-71 -395q-20 -107 -57.5 -168t-106.5 -94q-40 -18 -61 -20l-10 32q77 23 113 108q21 50 41 160l68 377q10 57 -1.5 69.5t-76.5 20.5l6 28h261z" /></g><g transform="matrix(.022,-0,0,-.022,10.307,15.825)"><path id="x2F" d="M368 703l-264 -866h-60l265 866h59z" /></g><g transform="matrix(.022,-0,0,-.022,19.542,15.825)"><path id="x1D713" d="M642 419q-50 -36 -71 -94q-28 -78 -68 -170q-39 -89 -114 -135q-34 -21 -83 -31l-45 -219l-31 -31q-8 7 -15 29.5t-2 45.5l35 172q-153 10 -153 169q0 28 6 84q7 68 7 88q0 48 -27 48q-18 0 -51 -28l-7 26q62 75 118 75q49 0 49 -90q0 -47 -5 -81q-10 -72 -10 -108
q0 -117 82 -133l87 455l62 19l7 -2l-99 -478q91 12 131 120q34 93 51 154q20 73 36 88q42 40 103 56z" /></g>

		
	
</svg> and <svg     style="vertical-align:-0.0pt;width:14.8125px;" id="M2" height="15.025" version="1.1" viewBox="0 0 14.8125 15.025" width="14.8125"  xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,14.975)"><path id="x3A5" d="M648 625l-6 -15q-6 1 -13 1q-42 0 -86.5 -30.5t-81.5 -88.5q-93 -143 -93 -298v-72q0 -60 15.5 -75.5t84.5 -19.5v-27h-284v27q67 4 83 19.5t16 75.5v78q0 163 -53 273q-64 136 -186 136q-18 0 -38 -3l-5 26q62 33 122 33q114 0 173 -150q33 -79 44 -206h5q21 106 59 180
q33 76 84.5 126t108.5 50q30 0 51 -40z" /></g>

		
	
</svg> 

Advances in High Energy Physics

Effects of Flavor Dependence on Weak Decays of and

Figure 1