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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4541 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{8}$ + ${ }M_{3}^{2}$ | 0.7543 | 0.9473 | 0.7962 | [M:[0.8235, 1.0, 1.0, 0.8235, 1.0, 0.7207, 0.8235, 1.0], q:[0.5883, 0.5883], qb:[0.4117, 0.5883], phi:[0.4559]] | [M:[[-4], [0], [0], [-4], [0], [5], [-4], [0]], q:[[2], [2]], qb:[[-2], [2]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{8}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$ | ${}M_{3}M_{5}$, ${ }M_{3}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{8}^{2}$ | -4 | t^2.162 + 3*t^2.47 + t^2.735 + 3*t^3. + t^4.324 + 3*t^4.368 + 3*t^4.632 + 7*t^4.897 + 6*t^4.941 + 3*t^5.162 + 3*t^5.206 + 7*t^5.47 + 3*t^5.735 - 4*t^6. + t^6.486 - t^6.53 + 3*t^6.794 + 6*t^6.838 + 7*t^7.059 + 8*t^7.103 + 3*t^7.324 + 18*t^7.368 + 10*t^7.411 + 10*t^7.632 + 6*t^7.676 + 9*t^7.897 + 12*t^7.941 - 10*t^8.162 + 7*t^8.206 - 3*t^8.427 - 12*t^8.47 + t^8.648 - t^8.692 - 4*t^8.735 + 3*t^8.957 - t^4.368/y - t^6.53/y - (3*t^6.838)/y - t^7.103/y + (4*t^7.632)/y + (4*t^7.897)/y + (3*t^7.941)/y + (3*t^8.162)/y + (4*t^8.206)/y + (9*t^8.47)/y - t^8.692/y + (3*t^8.735)/y - t^4.368*y - t^6.53*y - 3*t^6.838*y - t^7.103*y + 4*t^7.632*y + 4*t^7.897*y + 3*t^7.941*y + 3*t^8.162*y + 4*t^8.206*y + 9*t^8.47*y - t^8.692*y + 3*t^8.735*y | g1^5*t^2.162 + (3*t^2.47)/g1^4 + t^2.735/g1^2 + 3*t^3. + g1^10*t^4.324 + (3*t^4.368)/g1 + 3*g1*t^4.632 + 7*g1^3*t^4.897 + (6*t^4.941)/g1^8 + 3*g1^5*t^5.162 + (3*t^5.206)/g1^6 + (7*t^5.47)/g1^4 + (3*t^5.735)/g1^2 - 4*t^6. + g1^15*t^6.486 - g1^4*t^6.53 + 3*g1^6*t^6.794 + (6*t^6.838)/g1^5 + 7*g1^8*t^7.059 + (8*t^7.103)/g1^3 + 3*g1^10*t^7.324 + (18*t^7.368)/g1 + (10*t^7.411)/g1^12 + 10*g1*t^7.632 + (6*t^7.676)/g1^10 + 9*g1^3*t^7.897 + (12*t^7.941)/g1^8 - 10*g1^5*t^8.162 + (7*t^8.206)/g1^6 - 3*g1^7*t^8.427 - (12*t^8.47)/g1^4 + g1^20*t^8.648 - g1^9*t^8.692 - (4*t^8.735)/g1^2 + 3*g1^11*t^8.957 - t^4.368/(g1*y) - (g1^4*t^6.53)/y - (3*t^6.838)/(g1^5*y) - t^7.103/(g1^3*y) + (4*g1*t^7.632)/y + (4*g1^3*t^7.897)/y + (3*t^7.941)/(g1^8*y) + (3*g1^5*t^8.162)/y + (4*t^8.206)/(g1^6*y) + (9*t^8.47)/(g1^4*y) - (g1^9*t^8.692)/y + (3*t^8.735)/(g1^2*y) - (t^4.368*y)/g1 - g1^4*t^6.53*y - (3*t^6.838*y)/g1^5 - (t^7.103*y)/g1^3 + 4*g1*t^7.632*y + 4*g1^3*t^7.897*y + (3*t^7.941*y)/g1^8 + 3*g1^5*t^8.162*y + (4*t^8.206*y)/g1^6 + (9*t^8.47*y)/g1^4 - g1^9*t^8.692*y + (3*t^8.735*y)/g1^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
2482 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{8}$ | 0.7556 | 0.9503 | 0.7951 | [M:[0.7959, 1.0276, 0.9724, 0.851, 1.0, 0.7207, 0.8235, 0.9724], q:[0.6159, 0.5883], qb:[0.4117, 0.5607], phi:[0.4559]] | t^2.162 + t^2.388 + t^2.47 + t^2.553 + t^2.735 + 2*t^2.917 + t^3. + t^4.285 + t^4.324 + t^4.368 + t^4.45 + t^4.55 + t^4.632 + t^4.715 + t^4.732 + t^4.775 + t^4.814 + t^4.858 + 3*t^4.897 + 2*t^4.941 + t^4.98 + t^5.023 + t^5.063 + 2*t^5.079 + t^5.106 + t^5.123 + t^5.162 + t^5.206 + t^5.288 + 2*t^5.305 + 2*t^5.388 + 3*t^5.47 + 2*t^5.652 + t^5.735 + 2*t^5.834 - 3*t^6. - t^4.368/y - t^4.368*y | detail |