Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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4418 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ | 0.6321 | 0.8217 | 0.7693 | [M:[0.967, 1.099, 0.967, 0.901, 0.7418, 1.2582, 0.8077, 0.8077], q:[0.7418, 0.2912], qb:[0.4505, 0.4505], phi:[0.5165]] | [M:[[4], [-12], [4], [12], [1], [-1], [-7], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{7}$, ${ }M_{8}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{8}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }M_{8}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{3}M_{8}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{8}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | -1 | 2*t^2.225 + 2*t^2.423 + t^2.703 + 2*t^2.901 + t^3.297 + 2*t^3.775 + 3*t^4.253 + 3*t^4.451 + 4*t^4.648 + 3*t^4.846 + 2*t^4.928 + 6*t^5.126 + 4*t^5.324 + t^5.406 + 2*t^5.604 + 2*t^5.72 + 2*t^5.802 - t^6. + 4*t^6.198 + 4*t^6.478 + t^6.594 + 10*t^6.676 + 2*t^6.874 + 3*t^6.956 + 6*t^7.072 + 6*t^7.154 + 4*t^7.269 + 5*t^7.352 + 9*t^7.549 + 2*t^7.632 + 5*t^7.747 + 4*t^7.829 + 8*t^8.027 + t^8.109 + 3*t^8.143 - 2*t^8.225 + 2*t^8.307 - 6*t^8.423 + 7*t^8.505 + 6*t^8.621 + 2*t^8.703 + 2*t^8.901 - t^4.549/y - (2*t^6.973)/y + (5*t^7.648)/y + t^7.846/y + (2*t^7.928)/y + (8*t^8.126)/y + (4*t^8.324)/y + (2*t^8.522)/y + (2*t^8.604)/y + (2*t^8.72)/y + t^8.802/y - t^4.549*y - 2*t^6.973*y + 5*t^7.648*y + t^7.846*y + 2*t^7.928*y + 8*t^8.126*y + 4*t^8.324*y + 2*t^8.522*y + 2*t^8.604*y + 2*t^8.72*y + t^8.802*y | 2*g1*t^2.225 + (2*t^2.423)/g1^7 + g1^12*t^2.703 + 2*g1^4*t^2.901 + t^3.297/g1^12 + (2*t^3.775)/g1 + 3*g1^10*t^4.253 + 3*g1^2*t^4.451 + (4*t^4.648)/g1^6 + (3*t^4.846)/g1^14 + 2*g1^13*t^4.928 + 6*g1^5*t^5.126 + (4*t^5.324)/g1^3 + g1^24*t^5.406 + 2*g1^16*t^5.604 + (2*t^5.72)/g1^19 + 2*g1^8*t^5.802 - t^6. + (4*t^6.198)/g1^8 + 4*g1^11*t^6.478 + t^6.594/g1^24 + 10*g1^3*t^6.676 + (2*t^6.874)/g1^5 + 3*g1^22*t^6.956 + (6*t^7.072)/g1^13 + 6*g1^14*t^7.154 + (4*t^7.269)/g1^21 + 5*g1^6*t^7.352 + (9*t^7.549)/g1^2 + 2*g1^25*t^7.632 + (5*t^7.747)/g1^10 + 4*g1^17*t^7.829 + 8*g1^9*t^8.027 + g1^36*t^8.109 + (3*t^8.143)/g1^26 - 2*g1*t^8.225 + 2*g1^28*t^8.307 - (6*t^8.423)/g1^7 + 7*g1^20*t^8.505 + (6*t^8.621)/g1^15 + 2*g1^12*t^8.703 + 2*g1^4*t^8.901 - t^4.549/(g1^2*y) - (2*t^6.973)/(g1^9*y) + (5*t^7.648)/(g1^6*y) + t^7.846/(g1^14*y) + (2*g1^13*t^7.928)/y + (8*g1^5*t^8.126)/y + (4*t^8.324)/(g1^3*y) + (2*t^8.522)/(g1^11*y) + (2*g1^16*t^8.604)/y + (2*t^8.72)/(g1^19*y) + (g1^8*t^8.802)/y - (t^4.549*y)/g1^2 - (2*t^6.973*y)/g1^9 + (5*t^7.648*y)/g1^6 + (t^7.846*y)/g1^14 + 2*g1^13*t^7.928*y + 8*g1^5*t^8.126*y + (4*t^8.324*y)/g1^3 + (2*t^8.522*y)/g1^11 + 2*g1^16*t^8.604*y + (2*t^8.72*y)/g1^19 + g1^8*t^8.802*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
2393 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ | 0.6165 | 0.7954 | 0.7751 | [M:[0.9591, 1.1226, 0.9591, 0.8774, 0.7398, 1.2602, 0.8215], q:[0.7398, 0.3011], qb:[0.4387, 0.4387], phi:[0.5204]] | 2*t^2.219 + t^2.465 + t^2.632 + 2*t^2.877 + t^3.368 + t^3.535 + 2*t^3.781 + 3*t^4.194 + 3*t^4.439 + 2*t^4.684 + 2*t^4.852 + t^4.929 + 5*t^5.097 + t^5.264 + 2*t^5.342 + 2*t^5.51 + 4*t^5.755 + t^5.832 - t^4.561/y - t^4.561*y | detail |