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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8495 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1q_2$ + $ \phi_1^3q_2^2$ + $ \phi_1^4X_2$ | 0.9465 | 1.0057 | 0.9411 | [X:[1.7293, 1.4585], M:[1.0829, 0.6768], q:[0.3909, 0.797], qb:[], phi:[0.1354]] | [X:[[4], [8]], M:[[-16], [-10]], q:[[9], [3]], qb:[], phi:[[-2]]] | 1 | {a: 110200/116427, c: 117095/116427, X1: 1022/591, X2: 862/591, M1: 640/591, M2: 400/591, q1: 77/197, q2: 157/197, phi1: 80/591} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_2$, $ M_1$, $ \phi_1^3q_1^2$, $ q_1q_2$, $ M_2^2$, $ \phi_1^2q_1q_2$, $ X_2$, $ \phi_1q_2^2$, $ X_1$, $ M_1M_2$, $ M_2q_1q_2$ | . | -2 | t^2.03 + t^3.25 + 2*t^3.56 + t^4.06 + 2*t^4.38 + t^5.19 + t^5.28 + t^5.59 - 2*t^6. + t^6.09 + t^6.41 + t^6.5 + t^6.81 + 3*t^7.13 + t^7.31 + 3*t^7.62 + 3*t^7.94 - t^8.03 + t^8.12 + t^8.53 + 3*t^8.75 + 2*t^8.84 + t^7.62/y^2 - t^8.44/y^2 - t^3.41/y - t^4.22/y - t^5.44/y - t^6.25/y - t^6.65/y - t^6.97/y - (2*t^7.47)/y - (2*t^7.78)/y + t^8.19/y + t^8.59/y - t^8.69/y - t^3.41*y - t^4.22*y - t^5.44*y - t^6.25*y - t^6.65*y - t^6.97*y - 2*t^7.47*y - 2*t^7.78*y + t^8.19*y + t^8.59*y - t^8.69*y + t^7.62*y^2 - t^8.44*y^2 | t^2.03/g1^10 + t^3.25/g1^16 + 2*g1^12*t^3.56 + t^4.06/g1^20 + 2*g1^8*t^4.38 + g1^4*t^5.19 + t^5.28/g1^26 + g1^2*t^5.59 - 2*t^6. + t^6.09/g1^30 + t^6.41/g1^2 + t^6.5/g1^32 + t^6.81/g1^4 + 3*g1^24*t^7.13 + t^7.31/g1^36 + (3*t^7.62)/g1^8 + 3*g1^20*t^7.94 - t^8.03/g1^10 + t^8.12/g1^40 + t^8.53/g1^42 + 3*g1^16*t^8.75 + (2*t^8.84)/g1^14 + t^7.62/(g1^8*y^2) - t^8.44/(g1^12*y^2) - t^3.41/(g1^2*y) - t^4.22/(g1^6*y) - t^5.44/(g1^12*y) - t^6.25/(g1^16*y) - t^6.65/(g1^18*y) - (g1^10*t^6.97)/y - (2*t^7.47)/(g1^22*y) - (2*g1^6*t^7.78)/y + (g1^4*t^8.19)/y + (g1^2*t^8.59)/y - t^8.69/(g1^28*y) - (t^3.41*y)/g1^2 - (t^4.22*y)/g1^6 - (t^5.44*y)/g1^12 - (t^6.25*y)/g1^16 - (t^6.65*y)/g1^18 - g1^10*t^6.97*y - (2*t^7.47*y)/g1^22 - 2*g1^6*t^7.78*y + g1^4*t^8.19*y + g1^2*t^8.59*y - (t^8.69*y)/g1^28 + (t^7.62*y^2)/g1^8 - (t^8.44*y^2)/g1^12 |
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 |
---|---|---|---|---|---|---|---|---|---|
8228 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1q_2$ | 1.1778 | 1.3093 | 0.8996 | [X:[1.6457], M:[0.8448, 0.8858], q:[0.489, 0.4481], qb:[], phi:[0.1772]] | t^2.13 + t^2.53 + t^2.66 + t^2.81 + t^3.22 + t^3.87 + t^4.25 + t^4.28 + t^4.41 + t^4.53 + t^4.66 + t^4.78 + 2*t^4.94 + t^5.07 + t^5.19 + t^5.31 + 2*t^5.35 + t^5.47 + t^5.62 + t^5.75 - t^6. - t^3.53/y - t^4.59/y - t^5.66/y - t^3.53*y - t^4.59*y - t^5.66*y | detail |