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 |
---|---|---|---|---|---|---|---|---|---|
205 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ | 0.7556 | 0.9204 | 0.821 | [M:[0.7942, 0.7942, 0.7604], q:[0.586, 0.6198], qb:[0.6198, 0.586], phi:[0.3971]] | [M:[[-2, -2], [-2, -2], [-4, 0]], q:[[0, 2], [2, 0]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | t^2.281 + 3*t^2.383 + t^3.516 + 2*t^3.617 + t^4.562 + 3*t^4.664 + 3*t^4.707 + 6*t^4.765 + 4*t^4.809 + 3*t^4.91 + t^5.797 + t^5.899 - 2*t^6. - 4*t^6.101 + t^6.843 + 3*t^6.945 + 3*t^6.988 + t^7.032 + 6*t^7.046 + 9*t^7.09 + 2*t^7.134 + 10*t^7.148 + 8*t^7.191 + 2*t^7.235 + 5*t^7.293 + t^8.078 + t^8.18 + 3*t^8.223 - 5*t^8.281 + 3*t^8.325 - 12*t^8.383 - 9*t^8.484 - t^8.528 - t^4.191/y - t^6.472/y - (3*t^6.574)/y + (3*t^7.664)/y + (3*t^7.765)/y + (3*t^7.809)/y + t^7.91/y - t^8.753/y + t^8.797/y - (3*t^8.855)/y + (5*t^8.899)/y - (6*t^8.956)/y - t^4.191*y - t^6.472*y - 3*t^6.574*y + 3*t^7.664*y + 3*t^7.765*y + 3*t^7.809*y + t^7.91*y - t^8.753*y + t^8.797*y - 3*t^8.855*y + 5*t^8.899*y - 6*t^8.956*y | t^2.281/g1^4 + (3*t^2.383)/(g1^2*g2^2) + g2^4*t^3.516 + 2*g1^2*g2^2*t^3.617 + t^4.562/g1^8 + (3*t^4.664)/(g1^6*g2^2) + (3*g2^3*t^4.707)/g1 + (6*t^4.765)/(g1^4*g2^4) + 4*g1*g2*t^4.809 + (3*g1^3*t^4.91)/g2 + (g2^4*t^5.797)/g1^4 + (g2^2*t^5.899)/g1^2 - 2*t^6. - (4*g1^2*t^6.101)/g2^2 + t^6.843/g1^12 + (3*t^6.945)/(g1^10*g2^2) + (3*g2^3*t^6.988)/g1^5 + g2^8*t^7.032 + (6*t^7.046)/(g1^8*g2^4) + (9*g2*t^7.09)/g1^3 + 2*g1^2*g2^6*t^7.134 + (10*t^7.148)/(g1^6*g2^6) + (8*t^7.191)/(g1*g2) + 2*g1^4*g2^4*t^7.235 + (5*g1*t^7.293)/g2^3 + (g2^4*t^8.078)/g1^8 + (g2^2*t^8.18)/g1^6 + (3*g2^7*t^8.223)/g1 - (5*t^8.281)/g1^4 + 3*g1*g2^5*t^8.325 - (12*t^8.383)/(g1^2*g2^2) - (9*t^8.484)/g2^4 - g1^5*g2*t^8.528 - t^4.191/(g1*g2*y) - t^6.472/(g1^5*g2*y) - (3*t^6.574)/(g1^3*g2^3*y) + (3*t^7.664)/(g1^6*g2^2*y) + (3*t^7.765)/(g1^4*g2^4*y) + (3*g1*g2*t^7.809)/y + (g1^3*t^7.91)/(g2*y) - t^8.753/(g1^9*g2*y) + (g2^4*t^8.797)/(g1^4*y) - (3*t^8.855)/(g1^7*g2^3*y) + (5*g2^2*t^8.899)/(g1^2*y) - (6*t^8.956)/(g1^5*g2^5*y) - (t^4.191*y)/(g1*g2) - (t^6.472*y)/(g1^5*g2) - (3*t^6.574*y)/(g1^3*g2^3) + (3*t^7.664*y)/(g1^6*g2^2) + (3*t^7.765*y)/(g1^4*g2^4) + 3*g1*g2*t^7.809*y + (g1^3*t^7.91*y)/g2 - (t^8.753*y)/(g1^9*g2) + (g2^4*t^8.797*y)/g1^4 - (3*t^8.855*y)/(g1^7*g2^3) + (5*g2^2*t^8.899*y)/g1^2 - (6*t^8.956*y)/(g1^5*g2^5) |
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 |
---|---|---|---|---|---|---|---|---|
322 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ | 0.6999 | 0.852 | 0.8215 | [X:[], M:[0.9551932868590881, 0.9551932868590881, 1.0448067131409118], q:[0.5672100697113678, 0.47759664342954405], qb:[0.47759664342954405, 0.5672100697113678], phi:[0.47759664342954405]] | detail | ||
324 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.694 | 0.8536 | 0.813 | [M:[1.0, 1.0, 0.9459], q:[0.473, 0.527], qb:[0.527, 0.473], phi:[0.5]] | 2*t^2.838 + 5*t^3. + 3*t^4.338 + 4*t^4.5 + 3*t^4.662 + 3*t^5.675 + 6*t^5.838 + 6*t^6. - t^4.5/y - t^4.5*y | detail | |
325 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ | 0.7546 | 0.9174 | 0.8226 | [M:[0.7904, 0.7904, 0.7904], q:[0.6048, 0.6048], qb:[0.6048, 0.6048], phi:[0.3952]] | 4*t^2.371 + 3*t^3.629 + 10*t^4.743 + 10*t^4.814 - 4*t^6. - t^4.186/y - t^4.186*y | detail | |
326 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ | 0.7722 | 0.9495 | 0.8132 | [M:[0.7745, 0.7745, 0.7745, 0.7745], q:[0.6127, 0.6127], qb:[0.6127, 0.6127], phi:[0.3873]] | 5*t^2.324 + 2*t^3.676 + 15*t^4.647 + 10*t^4.838 - 6*t^6. - t^4.162/y - t^4.162*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
125 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0.7382 | 0.8885 | 0.8308 | [M:[0.8108, 0.8108], q:[0.5946, 0.5946], qb:[0.5946, 0.5946], phi:[0.4054]] | 3*t^2.432 + 4*t^3.568 + 10*t^4.784 + 6*t^4.865 - 4*t^6. - t^4.216/y - t^4.216*y | detail |