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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1578 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_3M_4$ + $ M_5q_2\tilde{q}_1$ + $ M_6\phi_1\tilde{q}_1\tilde{q}_2$ | 0.5831 | 0.7251 | 0.8041 | [X:[1.6364], M:[0.9091, 0.3636, 1.0909, 0.9091, 0.9091, 0.7273], q:[0.8182, 0.8182], qb:[0.2727, 0.6364], phi:[0.3636]] | [X:[[0]], M:[[0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 12417/21296, c: 7721/10648, X1: 18/11, M1: 10/11, M2: 4/11, M3: 12/11, M4: 10/11, M5: 10/11, M6: 8/11, q1: 9/11, q2: 9/11, qb1: 3/11, qb2: 7/11, phi1: 4/11} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_6$, $ \phi_1^2$, $ M_1$, $ M_4$, $ M_5$, $ \tilde{q}_1\tilde{q}_2$, $ M_6^2$, $ M_6\phi_1^2$, $ \phi_1^4$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ M_1M_6$, $ M_4M_6$, $ M_5M_6$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ q_1q_2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ X_1$, $ M_1^2$, $ M_1M_4$, $ M_4^2$, $ M_1M_5$, $ M_4M_5$, $ M_5^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$ | . | -4 | 2*t^2.18 + 4*t^2.73 + 5*t^4.36 + 9*t^4.91 + 8*t^5.45 - 4*t^6. + 3*t^6.55 + 17*t^7.09 + 14*t^7.64 + t^8.18 - 11*t^8.73 - t^4.09/y - (2*t^6.27)/y - (2*t^6.82)/y + (3*t^7.36)/y + (10*t^7.91)/y + (3*t^8.45)/y - t^4.09*y - 2*t^6.27*y - 2*t^6.82*y + 3*t^7.36*y + 10*t^7.91*y + 3*t^8.45*y | 2*t^2.18 + 4*t^2.73 + 5*t^4.36 + 9*t^4.91 + 8*t^5.45 - 4*t^6. + 3*t^6.55 + 17*t^7.09 + 14*t^7.64 + t^8.18 - 11*t^8.73 - t^4.09/y - (2*t^6.27)/y - (2*t^6.82)/y + (3*t^7.36)/y + (10*t^7.91)/y + (3*t^8.45)/y - t^4.09*y - 2*t^6.27*y - 2*t^6.82*y + 3*t^7.36*y + 10*t^7.91*y + 3*t^8.45*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 |
---|---|---|---|---|---|---|---|---|---|
1005 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_3M_4$ + $ M_5q_2\tilde{q}_1$ | 0.5632 | 0.6882 | 0.8184 | [X:[1.6364], M:[0.9091, 0.3636, 1.0909, 0.9091, 0.9091], q:[0.8182, 0.8182], qb:[0.2727, 0.6364], phi:[0.3636]] | t^2.18 + 4*t^2.73 + t^3.82 + 3*t^4.36 + 5*t^4.91 + 8*t^5.45 - 3*t^6. - t^4.09/y - t^4.09*y | detail | {a: 5997/10648, c: 916/1331, X1: 18/11, M1: 10/11, M2: 4/11, M3: 12/11, M4: 10/11, M5: 10/11, q1: 9/11, q2: 9/11, qb1: 3/11, qb2: 7/11, phi1: 4/11} |