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 |
|---|---|---|---|---|---|---|---|---|---|
| 4394 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{3}M_{5}$ + ${ }M_{5}M_{7}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{6}M_{8}$ | 0.5904 | 0.7513 | 0.7859 | [M:[0.7186, 1.1421, 0.9972, 0.7131, 1.0028, 1.2869, 0.9972, 0.7131], q:[0.9276, 0.3538], qb:[0.3593, 0.6434], phi:[0.429]] | [M:[[22], [-4], [-14], [-6], [14], [6], [-14], [-6]], q:[[-5], [-17]], qb:[[11], [3]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{8}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{8}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{8}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{8}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{7}^{2}$ | ${}$ | -3 | 2*t^2.139 + t^2.156 + 2*t^2.992 + t^3.41 + 2*t^3.426 + t^3.443 + 3*t^4.279 + 2*t^4.295 + t^4.312 + t^4.713 + 4*t^5.131 + 2*t^5.148 + 2*t^5.549 + 4*t^5.566 + 3*t^5.582 + t^5.599 + 2*t^5.983 - 3*t^6. - t^6.017 + 2*t^6.401 + 6*t^6.418 + 3*t^6.434 + 2*t^6.451 + t^6.468 + t^6.819 + t^6.836 + 2*t^6.852 + t^6.869 + t^6.886 + 4*t^7.27 + t^7.287 + t^7.303 + 3*t^7.688 + 6*t^7.705 + 3*t^7.721 + 3*t^7.738 + t^7.754 + 4*t^8.123 - 4*t^8.139 - 5*t^8.156 - t^8.172 + 4*t^8.541 + 8*t^8.557 + 4*t^8.574 + 3*t^8.59 + 2*t^8.607 + t^8.623 + 2*t^8.959 + 4*t^8.975 - 3*t^8.992 - t^4.287/y - t^6.426/y - t^6.443/y + (3*t^7.295)/y + (5*t^8.131)/y + (3*t^8.148)/y + (2*t^8.549)/y + (4*t^8.566)/y + (3*t^8.582)/y + t^8.983/y - t^4.287*y - t^6.426*y - t^6.443*y + 3*t^7.295*y + 5*t^8.131*y + 3*t^8.148*y + 2*t^8.549*y + 4*t^8.566*y + 3*t^8.582*y + t^8.983*y | (2*t^2.139)/g1^6 + g1^22*t^2.156 + (2*t^2.992)/g1^14 + t^3.41/g1^32 + (2*t^3.426)/g1^4 + g1^24*t^3.443 + (3*t^4.279)/g1^12 + 2*g1^16*t^4.295 + g1^44*t^4.312 + t^4.713/g1^2 + (4*t^5.131)/g1^20 + 2*g1^8*t^5.148 + (2*t^5.549)/g1^38 + (4*t^5.566)/g1^10 + 3*g1^18*t^5.582 + g1^46*t^5.599 + (2*t^5.983)/g1^28 - 3*t^6. - g1^28*t^6.017 + (2*t^6.401)/g1^46 + (6*t^6.418)/g1^18 + 3*g1^10*t^6.434 + 2*g1^38*t^6.451 + g1^66*t^6.468 + t^6.819/g1^64 + t^6.836/g1^36 + (2*t^6.852)/g1^8 + g1^20*t^6.869 + g1^48*t^6.886 + (4*t^7.27)/g1^26 + g1^2*t^7.287 + g1^30*t^7.303 + (3*t^7.688)/g1^44 + (6*t^7.705)/g1^16 + 3*g1^12*t^7.721 + 3*g1^40*t^7.738 + g1^68*t^7.754 + (4*t^8.123)/g1^34 - (4*t^8.139)/g1^6 - 5*g1^22*t^8.156 - g1^50*t^8.172 + (4*t^8.541)/g1^52 + (8*t^8.557)/g1^24 + 4*g1^4*t^8.574 + 3*g1^32*t^8.59 + 2*g1^60*t^8.607 + g1^88*t^8.623 + (2*t^8.959)/g1^70 + (4*t^8.975)/g1^42 - (3*t^8.992)/g1^14 - (g1^2*t^4.287)/y - t^6.426/(g1^4*y) - (g1^24*t^6.443)/y + (3*g1^16*t^7.295)/y + (5*t^8.131)/(g1^20*y) + (3*g1^8*t^8.148)/y + (2*t^8.549)/(g1^38*y) + (4*t^8.566)/(g1^10*y) + (3*g1^18*t^8.582)/y + t^8.983/(g1^28*y) - g1^2*t^4.287*y - (t^6.426*y)/g1^4 - g1^24*t^6.443*y + 3*g1^16*t^7.295*y + (5*t^8.131*y)/g1^20 + 3*g1^8*t^8.148*y + (2*t^8.549*y)/g1^38 + (4*t^8.566*y)/g1^10 + 3*g1^18*t^8.582*y + (t^8.983*y)/g1^28 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2380 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{3}M_{5}$ + ${ }M_{5}M_{7}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 0.5702 | 0.713 | 0.7996 | [M:[0.7158, 1.1426, 0.999, 0.7139, 1.001, 1.2861, 0.999], q:[0.9282, 0.356], qb:[0.3579, 0.6431], phi:[0.4287]] | t^2.142 + t^2.147 + 2*t^2.997 + t^3.422 + 2*t^3.428 + t^3.434 + t^3.858 + t^4.283 + t^4.289 + t^4.295 + t^4.714 + 2*t^5.139 + 2*t^5.145 + t^5.563 + 2*t^5.569 + 2*t^5.575 + t^5.581 + 2*t^5.994 - 2*t^6. - t^4.286/y - t^4.286*y | detail |