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 |
|---|---|---|---|---|---|---|---|---|---|
| 58712 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}\phi_{1}q_{1}^{2}$ | 0.7053 | 0.9006 | 0.7831 | [M:[1.1797, 1.0237, 0.8203, 0.8203, 0.7187, 1.078, 0.8203, 0.7187], q:[0.4102, 0.4102], qb:[0.5661, 0.7695], phi:[0.461]] | [M:[[2], [-22], [-2], [-2], [8], [12], [-2], [8]], q:[[-1], [-1]], qb:[[23], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{8}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{8}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{8}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{8}\phi_{1}q_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ | -2 | 2*t^2.156 + 3*t^2.461 + t^2.929 + t^3.071 + t^3.234 + t^3.844 + t^4.007 + 5*t^4.312 + 6*t^4.617 + t^4.78 + 6*t^4.922 + 2*t^5.085 + 2*t^5.227 + 5*t^5.39 + t^5.532 + 3*t^5.695 + t^5.858 - 2*t^6. + t^6.142 + 3*t^6.163 + 2*t^6.305 + 9*t^6.468 - t^6.61 + 13*t^6.773 - t^6.915 + 3*t^6.936 + 9*t^7.078 + 8*t^7.241 + 9*t^7.383 + 9*t^7.546 + 2*t^7.688 + t^7.709 + 8*t^7.851 + 3*t^8.014 - t^8.156 + 2*t^8.298 + 8*t^8.319 - 10*t^8.461 + 2*t^8.603 + 16*t^8.624 - t^8.766 + 2*t^8.787 + 16*t^8.929 - t^4.383/y - (2*t^6.539)/y - (2*t^6.844)/y + (2*t^7.312)/y - t^7.454/y + (6*t^7.617)/y + (5*t^7.922)/y + (2*t^8.085)/y + (4*t^8.227)/y + (5*t^8.39)/y + (3*t^8.532)/y - t^4.383*y - 2*t^6.539*y - 2*t^6.844*y + 2*t^7.312*y - t^7.454*y + 6*t^7.617*y + 5*t^7.922*y + 2*t^8.085*y + 4*t^8.227*y + 5*t^8.39*y + 3*t^8.532*y | 2*g1^8*t^2.156 + (3*t^2.461)/g1^2 + g1^22*t^2.929 + t^3.071/g1^22 + g1^12*t^3.234 + t^3.844/g1^8 + g1^26*t^4.007 + 5*g1^16*t^4.312 + 6*g1^6*t^4.617 + g1^40*t^4.78 + (6*t^4.922)/g1^4 + 2*g1^30*t^5.085 + (2*t^5.227)/g1^14 + 5*g1^20*t^5.39 + t^5.532/g1^24 + 3*g1^10*t^5.695 + g1^44*t^5.858 - 2*t^6. + t^6.142/g1^44 + 3*g1^34*t^6.163 + (2*t^6.305)/g1^10 + 9*g1^24*t^6.468 - t^6.61/g1^20 + 13*g1^14*t^6.773 - t^6.915/g1^30 + 3*g1^48*t^6.936 + 9*g1^4*t^7.078 + 8*g1^38*t^7.241 + (9*t^7.383)/g1^6 + 9*g1^28*t^7.546 + (2*t^7.688)/g1^16 + g1^62*t^7.709 + 8*g1^18*t^7.851 + 3*g1^52*t^8.014 - g1^8*t^8.156 + (2*t^8.298)/g1^36 + 8*g1^42*t^8.319 - (10*t^8.461)/g1^2 + (2*t^8.603)/g1^46 + 16*g1^32*t^8.624 - t^8.766/g1^12 + 2*g1^66*t^8.787 + 16*g1^22*t^8.929 - t^4.383/(g1^6*y) - (2*g1^2*t^6.539)/y - (2*t^6.844)/(g1^8*y) + (2*g1^16*t^7.312)/y - t^7.454/(g1^28*y) + (6*g1^6*t^7.617)/y + (5*t^7.922)/(g1^4*y) + (2*g1^30*t^8.085)/y + (4*t^8.227)/(g1^14*y) + (5*g1^20*t^8.39)/y + (3*t^8.532)/(g1^24*y) - (t^4.383*y)/g1^6 - 2*g1^2*t^6.539*y - (2*t^6.844*y)/g1^8 + 2*g1^16*t^7.312*y - (t^7.454*y)/g1^28 + 6*g1^6*t^7.617*y + (5*t^7.922*y)/g1^4 + 2*g1^30*t^8.085*y + (4*t^8.227*y)/g1^14 + 5*g1^20*t^8.39*y + (3*t^8.532*y)/g1^24 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 56797 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{7}$ | 0.6852 | 0.8626 | 0.7944 | [M:[1.1802, 1.0183, 0.8198, 0.8198, 0.7206, 1.0809, 0.8198], q:[0.4099, 0.4099], qb:[0.5718, 0.7702], phi:[0.4595]] | t^2.162 + 3*t^2.46 + t^2.945 + t^3.055 + t^3.243 + 2*t^3.838 + t^4.026 + 3*t^4.324 + 3*t^4.621 + t^4.809 + 6*t^4.919 + t^5.107 + t^5.217 + 4*t^5.405 + t^5.514 + 3*t^5.702 + t^5.89 - 2*t^6. - t^4.379/y - t^4.379*y | detail |