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 |
---|---|---|---|---|---|---|---|---|---|
60971 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.4063 | 1.6229 | 0.8666 | [X:[1.2727], M:[0.9091, 1.2727, 0.7174], q:[0.3595, 0.5512], qb:[0.3677, 0.5397], phi:[0.3636]] | [X:[[0, 0]], M:[[0, 0], [0, 0], [-1, 1]], q:[[-1, 0], [0, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }X_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{3}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{3}X_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | ${}$ | -2 | t^2.15 + t^2.7 + t^2.73 + t^2.76 + 2*t^3.27 + t^3.79 + 2*t^3.82 + t^4.3 + 2*t^4.36 + t^4.85 + 2*t^4.88 + t^4.9 + t^4.91 + t^4.92 + t^4.94 + t^5.4 + 3*t^5.43 + 3*t^5.45 + t^5.48 + t^5.51 + t^5.94 + 4*t^5.97 + t^5.99 - 2*t^6. + t^6.01 + 2*t^6.03 + t^6.46 + t^6.49 + t^6.51 + 4*t^6.52 + 6*t^6.55 + t^6.57 + t^6.58 + t^7. + 2*t^7.03 + t^7.05 + 5*t^7.06 + t^7.08 + 3*t^7.09 + t^7.1 - t^7.11 + 2*t^7.12 + t^7.55 + 5*t^7.58 + t^7.6 + 5*t^7.61 + 7*t^7.64 + 2*t^7.66 + t^7.7 + 2*t^8.09 + 4*t^8.12 + 2*t^8.13 + 4*t^8.15 + 3*t^8.17 + 3*t^8.18 + 3*t^8.19 - t^8.2 + 4*t^8.21 - t^8.22 + 2*t^8.23 + t^8.27 + t^8.61 + t^8.64 + t^8.66 + 6*t^8.67 + 2*t^8.69 + 2*t^8.7 + 3*t^8.71 + 6*t^8.73 + 2*t^8.75 - 3*t^8.76 - t^8.78 + 2*t^8.79 - t^4.09/y - t^5.18/y - t^6.24/y - t^6.79/y - t^6.82/y - t^6.85/y - t^7.33/y - t^7.36/y + t^7.85/y - t^7.91/y - t^8.4/y + (3*t^8.43)/y - t^8.45/y + t^8.48/y + (2*t^8.97)/y - t^4.09*y - t^5.18*y - t^6.24*y - t^6.79*y - t^6.82*y - t^6.85*y - t^7.33*y - t^7.36*y + t^7.85*y - t^7.91*y - t^8.4*y + 3*t^8.43*y - t^8.45*y + t^8.48*y + 2*t^8.97*y | (g2*t^2.15)/g1 + (g2*t^2.7)/g1 + t^2.73 + (g1*t^2.76)/g2 + 2*t^3.27 + (g2*t^3.79)/g1 + 2*t^3.82 + (g2^2*t^4.3)/g1^2 + 2*t^4.36 + (g2^2*t^4.85)/g1^2 + (2*g2*t^4.88)/g1 + t^4.9/(g1^2*g2) + t^4.91 + g1^2*g2*t^4.92 + (g1*t^4.94)/g2 + (g2^2*t^5.4)/g1^2 + (2*g2*t^5.43)/g1 + g1*g2^2*t^5.43 + 3*t^5.45 + t^5.48/(g1*g2^2) + (g1^2*t^5.51)/g2^2 + (g2^2*t^5.94)/g1^2 + (4*g2*t^5.97)/g1 + t^5.99/(g1^2*g2) - 2*t^6. + g1^2*g2*t^6.01 + (2*g1*t^6.03)/g2 + (g2^3*t^6.46)/g1^3 + (g2^2*t^6.49)/g1^2 + t^6.51/g1^3 + (3*g2*t^6.52)/g1 + g1*g2^2*t^6.52 + 6*t^6.55 + t^6.57/(g1*g2^2) + g1^3*t^6.58 + (g2^3*t^7.)/g1^3 + (2*g2^2*t^7.03)/g1^2 + t^7.05/g1^3 + (5*g2*t^7.06)/g1 + t^7.08/(g1^2*g2) + 3*t^7.09 + g1^2*g2*t^7.1 - t^7.11/(g1*g2^2) + (2*g1*t^7.12)/g2 + (g2^3*t^7.55)/g1^3 + (4*g2^2*t^7.58)/g1^2 + g2^3*t^7.58 + t^7.6/g1^3 + (3*g2*t^7.61)/g1 + 2*g1*g2^2*t^7.61 + 8*t^7.64 - g1^2*g2*t^7.64 + (2*t^7.66)/(g1*g2^2) + g1^3*t^7.67 - (g1*t^7.67)/g2 + (g1^2*t^7.7)/g2^2 + (2*g2^3*t^8.09)/g1^3 + (4*g2^2*t^8.12)/g1^2 + 2*g2^3*t^8.13 + (4*g2*t^8.15)/g1 + (3*t^8.17)/(g1^2*g2) + 3*t^8.18 + 3*g1^2*g2*t^8.19 - t^8.2/(g1*g2^2) + (4*g1*t^8.21)/g2 - g1^3*t^8.22 + (2*t^8.23)/g2^3 + (g1^3*t^8.27)/g2^3 + (g2^4*t^8.61)/g1^4 + (g2^3*t^8.64)/g1^3 + (g2*t^8.66)/g1^4 + (6*g2^2*t^8.67)/g1^2 + (2*t^8.69)/g1^3 + (2*g2*t^8.7)/g1 + 3*g1*g2^2*t^8.71 + 6*t^8.73 + (2*t^8.75)/(g1*g2^2) + g1^3*t^8.76 - (4*g1*t^8.76)/g2 - t^8.78/g2^3 + (2*g1^2*t^8.79)/g2^2 - t^4.09/y - t^5.18/y - (g2*t^6.24)/(g1*y) - (g2*t^6.79)/(g1*y) - t^6.82/y - (g1*t^6.85)/(g2*y) - (g2*t^7.33)/(g1*y) - t^7.36/y + (g2^2*t^7.85)/(g1^2*y) - t^7.91/y - (g2^2*t^8.4)/(g1^2*y) + (3*g2*t^8.43)/(g1*y) - t^8.45/y + (g1*t^8.48)/(g2*y) + (2*g2*t^8.97)/(g1*y) - t^4.09*y - t^5.18*y - (g2*t^6.24*y)/g1 - (g2*t^6.79*y)/g1 - t^6.82*y - (g1*t^6.85*y)/g2 - (g2*t^7.33*y)/g1 - t^7.36*y + (g2^2*t^7.85*y)/g1^2 - t^7.91*y - (g2^2*t^8.4*y)/g1^2 + (3*g2*t^8.43*y)/g1 - t^8.45*y + (g1*t^8.48*y)/g2 + (2*g2*t^8.97*y)/g1 |
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 |
---|
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 |
---|
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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
57959 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.3863 | 1.5852 | 0.8745 | [X:[1.2727], M:[0.9091, 1.2727], q:[0.3636, 0.5455], qb:[0.3636, 0.5455], phi:[0.3636]] | 3*t^2.73 + 2*t^3.27 + 4*t^3.82 + 2*t^4.36 + 4*t^4.91 + 7*t^5.45 + 4*t^6. - t^4.09/y - t^5.18/y - t^4.09*y - t^5.18*y | detail | {a: 29523/21296, c: 16879/10648, X1: 14/11, M1: 10/11, M2: 14/11, q1: 4/11, q2: 6/11, qb1: 4/11, qb2: 6/11, phi1: 4/11} |