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 |
|---|---|---|---|---|---|---|---|---|---|
| 1159 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6969 | 0.8688 | 0.8021 | [M:[0.9948, 1.127, 0.9339, 0.873, 0.7513, 0.7513], q:[0.7817, 0.4061], qb:[0.5992, 0.4669], phi:[0.4365]] | [M:[[32], [-12], [22], [12], [-8], [-8]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{6}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{6}q_{1}q_{2}$, ${ }M_{1}^{2}$ | ${}$ | -3 | 2*t^2.254 + 2*t^2.619 + t^2.802 + t^2.984 + t^3.563 + t^3.929 + t^4.111 + t^4.143 + t^4.325 + 4*t^4.508 + 4*t^4.873 + t^4.904 + 2*t^5.056 + 5*t^5.238 + t^5.421 + 2*t^5.603 + t^5.786 + t^5.817 + t^5.969 - 3*t^6. + 2*t^6.183 + 2*t^6.365 + t^6.397 + 2*t^6.548 + t^6.579 + 2*t^6.73 + 6*t^6.762 + t^6.913 + t^6.944 + t^7.096 + 7*t^7.127 + 2*t^7.158 + 2*t^7.31 + 8*t^7.492 + t^7.524 + 2*t^7.675 + 8*t^7.857 - t^7.889 + 4*t^8.04 + t^8.071 + 5*t^8.222 - 7*t^8.254 + 2*t^8.405 + t^8.437 + t^8.468 + 2*t^8.588 - 3*t^8.619 + t^8.651 + t^8.77 + t^8.833 + t^8.953 - t^8.984 - t^4.31/y - (2*t^6.563)/y - t^6.929/y - t^7.111/y - t^7.294/y + t^7.325/y + (2*t^7.508)/y + t^7.69/y + (4*t^7.873)/y + (4*t^8.056)/y + (3*t^8.238)/y + (2*t^8.421)/y + (2*t^8.603)/y + t^8.786/y - t^8.817/y - t^4.31*y - 2*t^6.563*y - t^6.929*y - t^7.111*y - t^7.294*y + t^7.325*y + 2*t^7.508*y + t^7.69*y + 4*t^7.873*y + 4*t^8.056*y + 3*t^8.238*y + 2*t^8.421*y + 2*t^8.603*y + t^8.786*y - t^8.817*y | (2*t^2.254)/g1^8 + 2*g1^12*t^2.619 + g1^22*t^2.802 + g1^32*t^2.984 + t^3.563/g1^2 + g1^18*t^3.929 + g1^28*t^4.111 + t^4.143/g1^36 + t^4.325/g1^26 + (4*t^4.508)/g1^16 + 4*g1^4*t^4.873 + t^4.904/g1^60 + 2*g1^14*t^5.056 + 5*g1^24*t^5.238 + g1^34*t^5.421 + 2*g1^44*t^5.603 + g1^54*t^5.786 + t^5.817/g1^10 + g1^64*t^5.969 - 3*t^6. + 2*g1^10*t^6.183 + 2*g1^20*t^6.365 + t^6.397/g1^44 + 2*g1^30*t^6.548 + t^6.579/g1^34 + 2*g1^40*t^6.73 + (6*t^6.762)/g1^24 + g1^50*t^6.913 + t^6.944/g1^14 + g1^60*t^7.096 + (7*t^7.127)/g1^4 + (2*t^7.158)/g1^68 + 2*g1^6*t^7.31 + 8*g1^16*t^7.492 + t^7.524/g1^48 + 2*g1^26*t^7.675 + 8*g1^36*t^7.857 - t^7.889/g1^28 + 4*g1^46*t^8.04 + t^8.071/g1^18 + 5*g1^56*t^8.222 - (7*t^8.254)/g1^8 + 2*g1^66*t^8.405 + g1^2*t^8.437 + t^8.468/g1^62 + 2*g1^76*t^8.588 - 3*g1^12*t^8.619 + t^8.651/g1^52 + g1^86*t^8.77 + t^8.833/g1^42 + g1^96*t^8.953 - g1^32*t^8.984 - (g1^6*t^4.31)/y - (2*t^6.563)/(g1^2*y) - (g1^18*t^6.929)/y - (g1^28*t^7.111)/y - (g1^38*t^7.294)/y + t^7.325/(g1^26*y) + (2*t^7.508)/(g1^16*y) + t^7.69/(g1^6*y) + (4*g1^4*t^7.873)/y + (4*g1^14*t^8.056)/y + (3*g1^24*t^8.238)/y + (2*g1^34*t^8.421)/y + (2*g1^44*t^8.603)/y + (g1^54*t^8.786)/y - t^8.817/(g1^10*y) - g1^6*t^4.31*y - (2*t^6.563*y)/g1^2 - g1^18*t^6.929*y - g1^28*t^7.111*y - g1^38*t^7.294*y + (t^7.325*y)/g1^26 + (2*t^7.508*y)/g1^16 + (t^7.69*y)/g1^6 + 4*g1^4*t^7.873*y + 4*g1^14*t^8.056*y + 3*g1^24*t^8.238*y + 2*g1^34*t^8.421*y + 2*g1^44*t^8.603*y + g1^54*t^8.786*y - (t^8.817*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 709 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ | 0.6779 | 0.8345 | 0.8124 | [M:[0.9891, 1.1291, 0.93, 0.8709, 0.7527], q:[0.7823, 0.4059], qb:[0.605, 0.465], phi:[0.4355]] | t^2.258 + 2*t^2.613 + t^2.79 + t^2.967 + t^3.565 + t^3.742 + t^3.919 + t^4.096 + t^4.162 + t^4.339 + 2*t^4.516 + 2*t^4.871 + t^4.936 + t^5.048 + 4*t^5.226 + t^5.403 + 2*t^5.58 + t^5.757 + t^5.935 - 2*t^6. - t^4.306/y - t^4.306*y | detail |