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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47115 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6447 | 0.8471 | 0.7611 | [M:[0.9845, 0.7772, 1.0466, 0.7461, 0.7461], q:[0.7461, 0.2694], qb:[0.4767, 0.4767], phi:[0.5078]] | [M:[[4], [-7], [-12], [1], [1]], 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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${}M_{4}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}$ | -4 | 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^6.093 + 2*t^6.187 + 3*t^6.28 + 9*t^6.622 + 20*t^6.715 + 8*t^6.808 + 2*t^6.902 + t^6.995 + t^7.337 + 8*t^7.43 + 12*t^7.523 + 17*t^7.617 + 7*t^7.71 + 2*t^7.803 + t^8.052 + 4*t^8.145 - 16*t^8.238 - 2*t^8.332 + 7*t^8.425 + 10*t^8.518 + 3*t^8.611 + 5*t^8.767 + 18*t^8.86 + 27*t^8.953 - t^4.523/y - (2*t^6.762)/y - t^6.855/y + t^7.383/y + (6*t^7.477)/y + (4*t^7.57)/y - t^7.663/y + (5*t^8.192)/y + (7*t^8.285)/y + (9*t^8.378)/y + (2*t^8.471)/y + (4*t^8.907)/y - t^4.523*y - 2*t^6.762*y - t^6.855*y + t^7.383*y + 6*t^7.477*y + 4*t^7.57*y - t^7.663*y + 5*t^8.192*y + 7*t^8.285*y + 9*t^8.378*y + 2*t^8.471*y + 4*t^8.907*y | 4*g1*t^2.238 + t^2.332/g1^7 + g1^4*t^2.953 + t^3.047/g1^4 + (2*t^3.14)/g1^12 + g1^7*t^3.668 + 3*g1^10*t^4.383 + 10*g1^2*t^4.477 + (4*t^4.57)/g1^6 + t^4.663/g1^14 + 4*g1^5*t^5.192 + (5*t^5.285)/g1^3 + (7*t^5.378)/g1^11 + (2*t^5.471)/g1^19 + 4*g1^8*t^5.907 - 4*t^6. + t^6.093/g1^8 + (2*t^6.187)/g1^16 + (3*t^6.28)/g1^24 + 9*g1^11*t^6.622 + 20*g1^3*t^6.715 + (8*t^6.808)/g1^5 + (2*t^6.902)/g1^13 + t^6.995/g1^21 + g1^14*t^7.337 + 8*g1^6*t^7.43 + (12*t^7.523)/g1^2 + (17*t^7.617)/g1^10 + (7*t^7.71)/g1^18 + (2*t^7.803)/g1^26 + g1^17*t^8.052 + 4*g1^9*t^8.145 - 16*g1*t^8.238 - (2*t^8.332)/g1^7 + (7*t^8.425)/g1^15 + (10*t^8.518)/g1^23 + (3*t^8.611)/g1^31 + 5*g1^20*t^8.767 + 18*g1^12*t^8.86 + 27*g1^4*t^8.953 - t^4.523/(g1^2*y) - (2*t^6.762)/(g1*y) - t^6.855/(g1^9*y) + (g1^10*t^7.383)/y + (6*g1^2*t^7.477)/y + (4*t^7.57)/(g1^6*y) - t^7.663/(g1^14*y) + (5*g1^5*t^8.192)/y + (7*t^8.285)/(g1^3*y) + (9*t^8.378)/(g1^11*y) + (2*t^8.471)/(g1^19*y) + (4*g1^8*t^8.907)/y - (t^4.523*y)/g1^2 - (2*t^6.762*y)/g1 - (t^6.855*y)/g1^9 + g1^10*t^7.383*y + 6*g1^2*t^7.477*y + (4*t^7.57*y)/g1^6 - (t^7.663*y)/g1^14 + 5*g1^5*t^8.192*y + (7*t^8.285*y)/g1^3 + (9*t^8.378*y)/g1^11 + (2*t^8.471*y)/g1^19 + 4*g1^8*t^8.907*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 |
---|---|---|---|---|---|---|---|---|---|
46445 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6255 | 0.812 | 0.7702 | [M:[0.9852, 0.7759, 1.0444, 0.7463], q:[0.7463, 0.2685], qb:[0.4778, 0.4778], phi:[0.5074]] | 3*t^2.239 + t^2.328 + t^2.956 + t^3.044 + 2*t^3.133 + t^3.672 + t^3.761 + 3*t^4.389 + 6*t^4.478 + 3*t^4.567 + t^4.655 + 3*t^5.195 + 4*t^5.283 + 5*t^5.372 + 2*t^5.461 + 3*t^5.911 - t^6. - t^4.522/y - t^4.522*y | detail |