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 |
|---|---|---|---|---|---|---|---|---|---|
| 2388 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{7}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ | 0.5703 | 0.7124 | 0.8005 | [X:[1.5726], M:[1.2822, 1.1452, 0.4274, 0.9919, 0.7178, 1.0081, 0.7178], q:[0.367, 0.3508], qb:[0.6411, 0.9315], phi:[0.4274]] | [X:[[2]], M:[[-6], [4], [-2], [-14], [6], [14], [6]], q:[[17], [-11]], qb:[[-3], [5]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{5}\phi_{1}q_{1}q_{2}$, ${ }M_{7}\phi_{1}q_{1}q_{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$ | ${}$ | -2 | 2*t^2.153 + t^2.976 + t^3.024 + t^3.387 + 2*t^3.436 + t^3.484 + t^3.895 + 3*t^4.307 + t^4.718 + 2*t^5.129 + 2*t^5.178 + t^5.54 + 3*t^5.589 + 2*t^5.637 - 2*t^6. + 2*t^6.049 + t^6.363 + t^6.411 + 5*t^6.46 + t^6.508 + t^6.774 + 3*t^6.871 + 2*t^6.92 + t^6.968 - t^7.234 + t^7.282 + 3*t^7.331 + t^7.379 + 3*t^7.742 + 4*t^7.791 - 4*t^8.153 + 3*t^8.202 + t^8.516 + 6*t^8.613 + 2*t^8.662 + t^8.927 - 4*t^8.976 - t^4.282/y - t^6.436/y + t^7.307/y + (3*t^8.129)/y + (2*t^8.178)/y + (2*t^8.54)/y + (3*t^8.589)/y + (2*t^8.637)/y - t^4.282*y - t^6.436*y + t^7.307*y + 3*t^8.129*y + 2*t^8.178*y + 2*t^8.54*y + 3*t^8.589*y + 2*t^8.637*y | 2*g1^6*t^2.153 + t^2.976/g1^14 + g1^14*t^3.024 + t^3.387/g1^24 + 2*g1^4*t^3.436 + g1^32*t^3.484 + g1^22*t^3.895 + 3*g1^12*t^4.307 + g1^2*t^4.718 + (2*t^5.129)/g1^8 + 2*g1^20*t^5.178 + t^5.54/g1^18 + 3*g1^10*t^5.589 + 2*g1^38*t^5.637 - 2*t^6. + 2*g1^28*t^6.049 + t^6.363/g1^38 + t^6.411/g1^10 + 5*g1^18*t^6.46 + g1^46*t^6.508 + t^6.774/g1^48 + 3*g1^8*t^6.871 + 2*g1^36*t^6.92 + g1^64*t^6.968 - t^7.234/g1^30 + t^7.282/g1^2 + 3*g1^26*t^7.331 + g1^54*t^7.379 + 3*g1^16*t^7.742 + 4*g1^44*t^7.791 - 4*g1^6*t^8.153 + 3*g1^34*t^8.202 + t^8.516/g1^32 + 6*g1^24*t^8.613 + 2*g1^52*t^8.662 + t^8.927/g1^42 - (4*t^8.976)/g1^14 - t^4.282/(g1^2*y) - (g1^4*t^6.436)/y + (g1^12*t^7.307)/y + (3*t^8.129)/(g1^8*y) + (2*g1^20*t^8.178)/y + (2*t^8.54)/(g1^18*y) + (3*g1^10*t^8.589)/y + (2*g1^38*t^8.637)/y - (t^4.282*y)/g1^2 - g1^4*t^6.436*y + g1^12*t^7.307*y + (3*t^8.129*y)/g1^8 + 2*g1^20*t^8.178*y + (2*t^8.54*y)/g1^18 + 3*g1^10*t^8.589*y + 2*g1^38*t^8.637*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 |
|---|---|---|---|---|---|---|---|---|
| 4408 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{7}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{4}M_{8}$ | 0.5705 | 0.7151 | 0.7978 | [X:[1.5698], M:[1.2907, 1.1395, 0.4302, 1.0116, 0.7093, 0.9884, 0.7093, 0.9884], q:[0.3431, 0.3662], qb:[0.6453, 0.9244], phi:[0.4302]] | 2*t^2.128 + 2*t^2.965 + t^3.349 + 2*t^3.419 + t^3.488 + t^3.803 + 3*t^4.256 + t^4.709 + 4*t^5.093 + 2*t^5.477 + 3*t^5.547 + t^5.616 + 4*t^5.93 - 3*t^6. - t^4.291/y - t^4.291*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1334 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{7}$ | 0.705 | 0.8667 | 0.8134 | [M:[1.0704, 1.0358, 0.858, 0.9988, 0.9296, 1.0012, 0.9296], q:[0.466, 0.4636], qb:[0.5352, 0.6068], phi:[0.4821]] | t^2.574 + 2*t^2.789 + t^2.996 + t^3.004 + t^3.107 + t^3.218 + t^4.228 + t^4.235 + t^4.242 + t^4.443 + t^4.45 + 2*t^4.658 + t^4.665 + t^4.872 + t^5.087 + t^5.148 + 2*t^5.363 + 3*t^5.578 + t^5.681 + 2*t^5.792 + 2*t^5.896 - 3*t^6. - t^4.446/y - t^4.446*y | detail |