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 |
|---|---|---|---|---|---|---|---|---|---|
| 5704 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{8}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}X_{1}$ + ${ }M_{4}X_{2}$ + ${ }M_{5}M_{9}$ | 0.598 | 0.7382 | 0.8101 | [X:[1.6118, 1.3787], M:[1.0876, 1.1456, 0.7574, 0.6213, 0.9515, 1.0485, 0.3882, 0.8544, 1.0485], q:[0.7864, 0.2621], qb:[0.6503, 0.5923], phi:[0.4272]] | [X:[[32], [10]], M:[[34], [-12], [20], [-10], [4], [-4], [-32], [12], [-4]], q:[[-3], [-1]], qb:[[-33], [13]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{9}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{9}$, ${ }M_{1}M_{3}$, ${ }M_{6}M_{8}$, ${ }M_{8}M_{9}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{9}\phi_{1}^{2}$, ${ }M_{1}M_{8}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -3 | t^2.272 + 2*t^2.563 + 2*t^3.146 + t^3.263 + t^3.845 + t^4.019 + t^4.136 + t^4.31 + t^4.544 + 2*t^4.835 + 3*t^5.127 + t^5.184 + 2*t^5.418 + t^5.535 + 3*t^5.709 + t^5.826 - 3*t^6. - t^6.174 + 2*t^6.291 + 4*t^6.408 + t^6.525 + t^6.582 + t^6.699 + t^6.816 + 2*t^7.108 + 4*t^7.399 + t^7.456 - t^7.573 + 6*t^7.69 + t^7.747 + t^7.807 - t^7.864 + 3*t^7.981 + 2*t^8.098 + t^8.272 + 2*t^8.329 + t^8.389 - 4*t^8.563 + 3*t^8.68 - 2*t^8.737 + t^8.798 + t^8.854 + 5*t^8.972 - t^4.282/y - t^6.554/y - t^6.845/y + t^7.019/y + t^7.136/y - t^7.427/y - t^7.544/y + t^7.718/y + (2*t^7.835)/y + t^8.009/y + t^8.127/y + (2*t^8.418)/y + t^8.535/y + (4*t^8.709)/y + t^8.826/y - t^4.282*y - t^6.554*y - t^6.845*y + t^7.019*y + t^7.136*y - t^7.427*y - t^7.544*y + t^7.718*y + 2*t^7.835*y + t^8.009*y + t^8.127*y + 2*t^8.418*y + t^8.535*y + 4*t^8.709*y + t^8.826*y | g1^20*t^2.272 + 2*g1^12*t^2.563 + (2*t^3.146)/g1^4 + g1^34*t^3.263 + g1^18*t^3.845 + t^4.019/g1^28 + g1^10*t^4.136 + t^4.31/g1^36 + g1^40*t^4.544 + 2*g1^32*t^4.835 + 3*g1^24*t^5.127 + t^5.184/g1^60 + 2*g1^16*t^5.418 + g1^54*t^5.535 + 3*g1^8*t^5.709 + g1^46*t^5.826 - 3*t^6. - t^6.174/g1^46 + (2*t^6.291)/g1^8 + 4*g1^30*t^6.408 + g1^68*t^6.525 + t^6.582/g1^16 + g1^22*t^6.699 + g1^60*t^6.816 + 2*g1^52*t^7.108 + 4*g1^44*t^7.399 + t^7.456/g1^40 - t^7.573/g1^2 + 6*g1^36*t^7.69 + t^7.747/g1^48 + g1^74*t^7.807 - t^7.864/g1^10 + 3*g1^28*t^7.981 + 2*g1^66*t^8.098 + g1^20*t^8.272 + (2*t^8.329)/g1^64 + g1^58*t^8.389 - 4*g1^12*t^8.563 + 3*g1^50*t^8.68 - (2*t^8.737)/g1^34 + g1^88*t^8.798 + g1^4*t^8.854 + 5*g1^42*t^8.972 - (g1^6*t^4.282)/y - (g1^26*t^6.554)/y - (g1^18*t^6.845)/y + t^7.019/(g1^28*y) + (g1^10*t^7.136)/y - (g1^2*t^7.427)/y - (g1^40*t^7.544)/y + t^7.718/(g1^6*y) + (2*g1^32*t^7.835)/y + t^8.009/(g1^14*y) + (g1^24*t^8.127)/y + (2*g1^16*t^8.418)/y + (g1^54*t^8.535)/y + (4*g1^8*t^8.709)/y + (g1^46*t^8.826)/y - g1^6*t^4.282*y - g1^26*t^6.554*y - g1^18*t^6.845*y + (t^7.019*y)/g1^28 + g1^10*t^7.136*y - g1^2*t^7.427*y - g1^40*t^7.544*y + (t^7.718*y)/g1^6 + 2*g1^32*t^7.835*y + (t^8.009*y)/g1^14 + g1^24*t^8.127*y + 2*g1^16*t^8.418*y + g1^54*t^8.535*y + 4*g1^8*t^8.709*y + g1^46*t^8.826*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4207 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{8}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}X_{1}$ + ${ }M_{4}X_{2}$ | 0.6026 | 0.7461 | 0.8076 | [X:[1.6046, 1.3764], M:[1.0799, 1.1483, 0.7529, 0.6236, 0.9506, 1.0494, 0.3954, 0.8517], q:[0.7871, 0.2624], qb:[0.6578, 0.5894], phi:[0.4259]] | t^2.259 + 2*t^2.555 + t^2.852 + t^3.148 + t^3.24 + t^3.833 + t^4.038 + t^4.129 + t^4.335 + t^4.517 + 2*t^4.814 + 4*t^5.11 + t^5.224 + 3*t^5.407 + t^5.498 + 2*t^5.703 + t^5.795 - 2*t^6. - t^4.278/y - t^4.278*y | detail |