The Economical <svg style="vertical-align:-4.53427pt;width:232.325px;" id="M1" height="21.6875" version="1.1" viewBox="0 0 232.325 21.6875" width="232.325" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.975)"><path id="x1D446" d="M457 488l-30 -3q-17 148 -131 148q-53 0 -84.5 -34.5t-31.5 -82.5q0 -42 25.5 -72t74.5 -62l33 -22q63 -42 95 -85t32 -102q0 -84 -67 -137t-163 -53q-58 0 -113 22t-70 43l-4 152l27 4q4 -32 15 -62.5t31 -59.5t53.5 -47t76.5 -18q56 0 92 35t36 96q0 39 -25 70t-78 68
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<table>The one-loop corrections for the
mass matrix <svg height="14.2375" id="M1098" style="vertical-align:-3.13504pt" version="1.1" viewbox="0 0 24.549999 14.2375" width="24.549999" xmlns="http://www.w3.org/2000/svg">
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<tspan style="font-size: 12.50px; " x="0" y="0">𝑀</tspan>
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<text transform="matrix(1,0,0,-1,-59.38,60.66)">
<tspan style="font-size: 8.75px; " x="0" y="0">𝑅</tspan>
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</g>
</g>
</svg>.</table>

Advances in High Energy Physics

fig11

Figure 11

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l-110 215q-26 51 -44 63t-72 17l6 28h250l-6 -28l-27 -4q-30 -5 -35 -10t3 -27q17 -43 95 -190q70 78 154 185q15 21 10 29.5t-33 12.5l-30 4l5 28h236z" /></g></svg> Model 

Advances in High Energy Physics

The Economical Model

Figure 11