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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2940 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6627 | 0.88 | 0.7531 | [M:[0.9908, 1.0276, 0.7477, 0.7477, 0.7661, 0.7661], q:[0.7477, 0.2615], qb:[0.4862, 0.4862], phi:[0.5046]] | [M:[[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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${}M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$ | ${}$ | -5 | 4*t^2.243 + 2*t^2.298 + t^2.972 + t^3.028 + 2*t^3.083 + 3*t^4.431 + 10*t^4.486 + 8*t^4.541 + 3*t^4.597 + 4*t^5.216 + 6*t^5.271 + 8*t^5.326 + 4*t^5.381 - 5*t^6. + t^6.055 + 2*t^6.11 + 3*t^6.165 + 8*t^6.674 + 22*t^6.729 + 16*t^6.784 + 10*t^6.84 + 4*t^6.895 + 8*t^7.459 + 16*t^7.514 + 23*t^7.569 + 15*t^7.624 + 6*t^7.679 - 2*t^8.133 - 6*t^8.188 - 20*t^8.243 - 8*t^8.298 + 8*t^8.353 + 12*t^8.409 + 6*t^8.464 + 5*t^8.862 + 14*t^8.917 + 30*t^8.972 - t^4.514/y - (2*t^6.757)/y - (2*t^6.812)/y + t^7.431/y + (6*t^7.486)/y + (8*t^7.541)/y + (6*t^8.216)/y + (8*t^8.271)/y + (10*t^8.326)/y + (4*t^8.381)/y - t^4.514*y - 2*t^6.757*y - 2*t^6.812*y + t^7.431*y + 6*t^7.486*y + 8*t^7.541*y + 6*t^8.216*y + 8*t^8.271*y + 10*t^8.326*y + 4*t^8.381*y | 4*g1*t^2.243 + (2*t^2.298)/g1^7 + g1^4*t^2.972 + t^3.028/g1^4 + (2*t^3.083)/g1^12 + 3*g1^10*t^4.431 + 10*g1^2*t^4.486 + (8*t^4.541)/g1^6 + (3*t^4.597)/g1^14 + 4*g1^5*t^5.216 + (6*t^5.271)/g1^3 + (8*t^5.326)/g1^11 + (4*t^5.381)/g1^19 - 5*t^6. + t^6.055/g1^8 + (2*t^6.11)/g1^16 + (3*t^6.165)/g1^24 + 8*g1^11*t^6.674 + 22*g1^3*t^6.729 + (16*t^6.784)/g1^5 + (10*t^6.84)/g1^13 + (4*t^6.895)/g1^21 + 8*g1^6*t^7.459 + (16*t^7.514)/g1^2 + (23*t^7.569)/g1^10 + (15*t^7.624)/g1^18 + (6*t^7.679)/g1^26 - 2*g1^17*t^8.133 - 6*g1^9*t^8.188 - 20*g1*t^8.243 - (8*t^8.298)/g1^7 + (8*t^8.353)/g1^15 + (12*t^8.409)/g1^23 + (6*t^8.464)/g1^31 + 5*g1^20*t^8.862 + 14*g1^12*t^8.917 + 30*g1^4*t^8.972 - t^4.514/(g1^2*y) - (2*t^6.757)/(g1*y) - (2*t^6.812)/(g1^9*y) + (g1^10*t^7.431)/y + (6*g1^2*t^7.486)/y + (8*t^7.541)/(g1^6*y) + (6*g1^5*t^8.216)/y + (8*t^8.271)/(g1^3*y) + (10*t^8.326)/(g1^11*y) + (4*t^8.381)/(g1^19*y) - (t^4.514*y)/g1^2 - (2*t^6.757*y)/g1 - (2*t^6.812*y)/g1^9 + g1^10*t^7.431*y + 6*g1^2*t^7.486*y + (8*t^7.541*y)/g1^6 + 6*g1^5*t^8.216*y + (8*t^8.271*y)/g1^3 + (10*t^8.326*y)/g1^11 + (4*t^8.381*y)/g1^19 |
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 |
---|---|---|---|---|---|---|---|---|---|
1908 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6447 | 0.8471 | 0.7611 | [M:[0.9845, 1.0466, 0.7461, 0.7461, 0.7772], q:[0.7461, 0.2694], qb:[0.4767, 0.4767], phi:[0.5078]] | 4*t^2.238 + t^2.332 + t^2.953 + t^3.047 + 2*t^3.14 + t^3.668 + 3*t^4.383 + 10*t^4.477 + 4*t^4.57 + t^4.663 + 4*t^5.192 + 5*t^5.285 + 7*t^5.378 + 2*t^5.471 + 4*t^5.907 - 4*t^6. - t^4.523/y - t^4.523*y | detail |