Lower Mass Bound on the <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-0.2723999pt" id="M1" height="15.3681pt" version="1.1" viewBox="-0.0657574 -15.0957 21.9182 15.3681" width="21.9182pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-88" d="M962 650H739L732 622L760 619C812 613 819 604 798 552C760 457 671 267 606 131H604L511 638H480L237 131H233L183 554C177 607 183 614 226 619L248 622L257 650H24L17 622C88 615 92 611 103 524L173 -11H203L450 491H453L543 -11H575L839 529C882 609 886 613 953 622L962 650Z"/></g><g transform="matrix(.012,0,0,-0.012,16.723,-7.578)"><path id="g50-31" d="M310 541L304 571C290 586 211 619 185 610L80 76L131 52L310 541Z"/></g></svg> Mass via Neutrinoless Double Beta Decay in a 3-3-1 Model

<div>Novel 331 contribution for double beta decay due to light massive neutrinos.</div>

Advances in High Energy Physics

fig3

Figure 3

Figure 3: Lower Mass Bound on the <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-0.2723999pt" id="M1" height="15.3681pt" version="1.1" viewBox="-0.0657574 -15.0957 21.9182 15.3681" width="21.9182pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-88" d="M962 650H739L732 622L760 619C812 613 819 604 798 552C760 457 671 267 606 131H604L511 638H480L237 131H233L183 554C177 607 183 614 226 619L248 622L257 650H24L17 622C88 615 92 611 103 524L173 -11H203L450 491H453L543 -11H575L839 529C882 609 886 613 953 622L962 650Z"/></g><g transform="matrix(.012,0,0,-0.012,16.723,-7.578)"><path id="g50-31" d="M310 541L304 571C290 586 211 619 185 610L80 76L131 52L310 541Z"/></g></svg> Mass via Neutrinoless Double Beta Decay in a 3-3-1 Model 

Advances in High Energy Physics

Lower Mass Bound on the Mass via Neutrinoless Double Beta Decay in a 3-3-1 Model

Figure 3