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 |
|---|---|---|---|---|---|---|---|---|---|
| 1527 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6689 | 0.8376 | 0.7985 | [M:[1.0713, 0.8144, 1.0572, 0.8285, 1.1715, 0.7142], q:[0.5215, 0.4072], qb:[0.4213, 0.7643], phi:[0.4714]] | [M:[[-30], [22], [4], [-12], [12], [-20]], q:[[19], [11]], qb:[[-23], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$ | ${}M_{6}q_{1}\tilde{q}_{2}$ | 0 | t^2.143 + t^2.443 + t^2.486 + t^2.829 + t^3.171 + t^3.214 + t^3.514 + t^3.857 + t^3.9 + t^3.942 + t^4.2 + t^4.243 + t^4.285 + t^4.543 + t^4.586 + t^4.628 + t^4.886 + t^4.929 + 2*t^4.971 + t^5.272 + 2*t^5.314 + t^5.356 + t^5.615 + 3*t^5.657 + t^6.042 + t^6.085 + 2*t^6.343 + 3*t^6.385 + 3*t^6.428 + t^6.644 + 3*t^6.686 + 2*t^6.728 + 2*t^6.771 + t^6.987 + 2*t^7.029 + t^7.071 + 2*t^7.114 + t^7.156 + t^7.33 + 2*t^7.372 + t^7.414 + 3*t^7.457 + t^7.499 + t^7.715 + 2*t^7.757 + 4*t^7.8 + t^7.842 + t^7.884 + 2*t^8.058 + t^8.1 + t^8.143 + 2*t^8.185 + t^8.227 + t^8.401 - 2*t^8.443 + 2*t^8.486 + 2*t^8.528 + 3*t^8.57 + t^8.744 + t^8.786 + 2*t^8.829 + 4*t^8.871 + 3*t^8.913 - t^4.414/y - t^6.557/y - t^6.857/y + t^7.2/y + t^7.586/y + t^7.929/y + (2*t^7.971)/y + (2*t^8.272)/y + (2*t^8.314)/y + t^8.356/y + t^8.615/y + (3*t^8.657)/y + t^8.958/y - t^4.414*y - t^6.557*y - t^6.857*y + t^7.2*y + t^7.586*y + t^7.929*y + 2*t^7.971*y + 2*t^8.272*y + 2*t^8.314*y + t^8.356*y + t^8.615*y + 3*t^8.657*y + t^8.958*y | t^2.143/g1^20 + g1^22*t^2.443 + t^2.486/g1^12 + t^2.829/g1^4 + g1^4*t^3.171 + t^3.214/g1^30 + g1^12*t^3.514 + g1^20*t^3.857 + t^3.9/g1^14 + t^3.942/g1^48 + g1^28*t^4.2 + t^4.243/g1^6 + t^4.285/g1^40 + g1^36*t^4.543 + g1^2*t^4.586 + t^4.628/g1^32 + g1^44*t^4.886 + g1^10*t^4.929 + (2*t^4.971)/g1^24 + g1^18*t^5.272 + (2*t^5.314)/g1^16 + t^5.356/g1^50 + g1^26*t^5.615 + (3*t^5.657)/g1^8 + t^6.042/g1^34 + t^6.085/g1^68 + 2*g1^8*t^6.343 + (3*t^6.385)/g1^26 + (3*t^6.428)/g1^60 + g1^50*t^6.644 + 3*g1^16*t^6.686 + (2*t^6.728)/g1^18 + (2*t^6.771)/g1^52 + g1^58*t^6.987 + 2*g1^24*t^7.029 + t^7.071/g1^10 + (2*t^7.114)/g1^44 + t^7.156/g1^78 + g1^66*t^7.33 + 2*g1^32*t^7.372 + t^7.414/g1^2 + (3*t^7.457)/g1^36 + t^7.499/g1^70 + g1^40*t^7.715 + 2*g1^6*t^7.757 + (4*t^7.8)/g1^28 + t^7.842/g1^62 + t^7.884/g1^96 + 2*g1^48*t^8.058 + g1^14*t^8.1 + t^8.143/g1^20 + (2*t^8.185)/g1^54 + t^8.227/g1^88 + g1^56*t^8.401 - 2*g1^22*t^8.443 + (2*t^8.486)/g1^12 + (2*t^8.528)/g1^46 + (3*t^8.57)/g1^80 + g1^64*t^8.744 + g1^30*t^8.786 + (2*t^8.829)/g1^4 + (4*t^8.871)/g1^38 + (3*t^8.913)/g1^72 - t^4.414/(g1^2*y) - t^6.557/(g1^22*y) - (g1^20*t^6.857)/y + (g1^28*t^7.2)/y + (g1^2*t^7.586)/y + (g1^10*t^7.929)/y + (2*t^7.971)/(g1^24*y) + (2*g1^18*t^8.272)/y + (2*t^8.314)/(g1^16*y) + t^8.356/(g1^50*y) + (g1^26*t^8.615)/y + (3*t^8.657)/(g1^8*y) + (g1^34*t^8.958)/y - (t^4.414*y)/g1^2 - (t^6.557*y)/g1^22 - g1^20*t^6.857*y + g1^28*t^7.2*y + g1^2*t^7.586*y + g1^10*t^7.929*y + (2*t^7.971*y)/g1^24 + 2*g1^18*t^8.272*y + (2*t^8.314*y)/g1^16 + (t^8.356*y)/g1^50 + g1^26*t^8.615*y + (3*t^8.657*y)/g1^8 + g1^34*t^8.958*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 |
|---|---|---|---|---|---|---|---|---|
| 2621 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{2}M_{7}$ | 0.6538 | 0.8126 | 0.8046 | [M:[1.0497, 0.8302, 1.06, 0.8199, 1.1801, 0.6998, 1.1698], q:[0.5352, 0.4151], qb:[0.4048, 0.765], phi:[0.47]] | t^2.099 + t^2.46 + t^2.82 + t^3.149 + t^3.18 + t^3.509 + t^3.54 + t^3.838 + t^3.87 + t^3.901 + t^4.199 + t^4.23 + t^4.261 + t^4.559 + t^4.621 + 2*t^4.919 + t^5.248 + 2*t^5.279 + t^5.609 + 2*t^5.64 + t^5.938 + 2*t^5.969 - t^4.41/y - t^4.41*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 981 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ | 0.6487 | 0.7997 | 0.8112 | [M:[1.0791, 0.8087, 1.0561, 0.8316, 1.1684], q:[0.5166, 0.4043], qb:[0.4273, 0.764], phi:[0.4719]] | t^2.426 + t^2.495 + t^2.832 + t^3.168 + t^3.237 + t^3.505 + 2*t^3.842 + t^3.911 + t^3.98 + t^4.179 + t^4.247 + t^4.515 + t^4.852 + t^4.921 + t^4.99 + t^5.258 + t^5.327 + t^5.594 + 2*t^5.663 - t^6. - t^4.416/y - t^4.416*y | detail |