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 |
---|---|---|---|---|---|---|---|---|---|
61090 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.341 | 1.6124 | 0.8317 | [X:[], M:[0.8, 0.8573], q:[0.5524, 0.4951], qb:[0.2476, 0.3049], phi:[0.4]] | [X:[], M:[[0], [3]], q:[[1], [-2]], qb:[[-1], [2]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$ | ${}M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ 2}\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ 2}\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | 11 | t^2.23 + 4*t^2.4 + 2*t^2.57 + 3*t^3.6 + 2*t^3.77 + t^4.46 + 5*t^4.63 + 15*t^4.8 + 10*t^4.97 + 3*t^5.14 + 3*t^5.83 + 11*t^6. + 12*t^6.17 + 5*t^6.34 + t^6.68 + 5*t^6.86 + 16*t^7.03 + 40*t^7.2 + 35*t^7.37 + 18*t^7.54 + 4*t^7.72 + 4*t^8.06 + 8*t^8.23 + 28*t^8.4 + 37*t^8.57 + 26*t^8.74 + t^8.91 + 8*t^8.92 - t^4.2/y - t^5.4/y - t^6.43/y - (4*t^6.6)/y - (2*t^6.77)/y + (4*t^7.63)/y + (5*t^7.8)/y + (6*t^7.97)/y + t^8.14/y - t^8.66/y - t^8.83/y - t^4.2*y - t^5.4*y - t^6.43*y - 4*t^6.6*y - 2*t^6.77*y + 4*t^7.63*y + 5*t^7.8*y + 6*t^7.97*y + t^8.14*y - t^8.66*y - t^8.83*y | t^2.23/g1^3 + 4*t^2.4 + 2*g1^3*t^2.57 + 3*t^3.6 + 2*g1^3*t^3.77 + t^4.46/g1^6 + (5*t^4.63)/g1^3 + 15*t^4.8 + 10*g1^3*t^4.97 + 3*g1^6*t^5.14 + (3*t^5.83)/g1^3 + 11*t^6. + 12*g1^3*t^6.17 + 5*g1^6*t^6.34 + t^6.68/g1^9 + (5*t^6.86)/g1^6 + (16*t^7.03)/g1^3 + 40*t^7.2 + 35*g1^3*t^7.37 + 18*g1^6*t^7.54 + 4*g1^9*t^7.72 + (4*t^8.06)/g1^6 + (8*t^8.23)/g1^3 + 28*t^8.4 + 37*g1^3*t^8.57 + 26*g1^6*t^8.74 + t^8.91/g1^12 + 8*g1^9*t^8.92 - t^4.2/y - t^5.4/y - t^6.43/(g1^3*y) - (4*t^6.6)/y - (2*g1^3*t^6.77)/y + (4*t^7.63)/(g1^3*y) + (5*t^7.8)/y + (6*g1^3*t^7.97)/y + (g1^6*t^8.14)/y - t^8.66/(g1^6*y) - t^8.83/(g1^3*y) - t^4.2*y - t^5.4*y - (t^6.43*y)/g1^3 - 4*t^6.6*y - 2*g1^3*t^6.77*y + (4*t^7.63*y)/g1^3 + 5*t^7.8*y + 6*g1^3*t^7.97*y + g1^6*t^8.14*y - (t^8.66*y)/g1^6 - (t^8.83*y)/g1^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
58387 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.3293 | 1.5918 | 0.8351 | [X:[], M:[0.8], q:[0.56, 0.48], qb:[0.24, 0.32], phi:[0.4]] | t^2.16 + 4*t^2.4 + t^2.64 + t^3.36 + 3*t^3.6 + 2*t^3.84 + t^4.32 + 5*t^4.56 + 14*t^4.8 + 6*t^5.04 + t^5.28 + t^5.52 + 7*t^5.76 + 12*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail | {a: 13293/10000, c: 7959/5000, M1: 4/5, q1: 14/25, q2: 12/25, qb1: 6/25, qb2: 8/25, phi1: 2/5} |