Angular Dependence of <svg style="vertical-align:-3.69pt;width:15.4375px;" id="M1" height="20.075001" version="1.1" viewBox="0 0 15.4375 20.075001" width="15.4375" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.412)"><path id="x1D753" d="M395 685h117l-51 -223q86 0 140 -44.5t54 -124.5q0 -64 -29 -127q-36 -79 -108.5 -125t-164.5 -51l-44 -195h-117l45 195q-88 6 -140.5 56t-52.5 132q0 64 32 126q40 75 110.5 116.5t158.5 41.5zM453 423l-90 -393q58 12 108 74q49 63 63 128q5 23 5 53q0 49 -22 89
q-21 42 -64 49zM247 30l90 393q-72 -10 -125 -91q-52 -79 -52 -157q0 -55 22 -95.5t65 -49.5z" /></g></svg> Meson Production for Different Photon Beam Energies

<table>The source deformations and movements in the reaction plane corresponding to the different photon beam energies <svg height="18.362499" id="M62" style="vertical-align:-5.76984pt" version="1.1" viewbox="0 0 17.450001 18.362499" width="17.450001" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,11.113)"><path d="M609 650l-19 -162l-30 -2q2 69 -14 94q-9 18 -28.5 26t-74.5 8h-88q-30 0 -37 -6.5t-12 -36.5l-41 -212h103q48 0 69 5.5t32 19t26 50.5h29l-40 -198h-30q2 58 -11.5 70.5t-85.5 12.5h-99l-30 -167q-17 -87 3 -101q18 -15 111 -15q59 0 89 7t54 27q8 7 15.5 16t16 21.5
l14 20.5t15 23.5t13.5 21.5l29 -10q-52 -129 -71 -163h-500l6 28q66 4 83 17.5t28 73.5l77 409q11 61 -0.5 75.5t-78.5 18.5l10 28h467z" id="x1D438"></path></g>
<g transform="matrix(.012,-0,0,-.012,10.8,15.188)"><path d="M478 372q0 -39 -31 -97t-61 -98t-78 -98q-45 -55 -73 -102q-13 -79 -13 -197q-11 -11 -43.5 -25.5t-53.5 -15.5l-15 17q5 35 26 101.5t47 123.5q8 72 -1.5 174.5t-37.5 178.5q-14 37 -29 37q-20 0 -67 -65l-25 21q37 60 73 90.5t63 30.5q47 0 72 -112q13 -56 17.5 -141.5
t0.5 -143.5h2q155 193 155 297q0 26 -12 47q-5 8 -5 15q0 16 12.5 27t29.5 11q21 0 34 -21t13 -55z" id="x1D6FE"></path></g>
</svg>.</table>

Advances in High Energy Physics

fig6

Figure 6

Figure 6: Angular Dependence of <svg style="vertical-align:-3.69pt;width:15.4375px;" id="M1" height="20.075001" version="1.1" viewBox="0 0 15.4375 20.075001" width="15.4375" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.412)"><path id="x1D753" d="M395 685h117l-51 -223q86 0 140 -44.5t54 -124.5q0 -64 -29 -127q-36 -79 -108.5 -125t-164.5 -51l-44 -195h-117l45 195q-88 6 -140.5 56t-52.5 132q0 64 32 126q40 75 110.5 116.5t158.5 41.5zM453 423l-90 -393q58 12 108 74q49 63 63 128q5 23 5 53q0 49 -22 89
q-21 42 -64 49zM247 30l90 393q-72 -10 -125 -91q-52 -79 -52 -157q0 -55 22 -95.5t65 -49.5z" /></g></svg> Meson Production for Different Photon Beam Energies 

Advances in High Energy Physics

Angular Dependence of Meson Production for Different Photon Beam Energies

Figure 6