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 |
|---|---|---|---|---|---|---|---|---|---|
| 47009 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}^{2}$ | 0.7092 | 0.8704 | 0.8148 | [M:[0.8409, 1.0, 1.053, 0.8939, 1.0], q:[0.5265, 0.6326], qb:[0.4735, 0.4735], phi:[0.4735]] | [M:[[6], [0], [-2], [4], [0]], q:[[-1], [-5]], qb:[[1], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{2}M_{5}$, ${ }M_{4}q_{2}\tilde{q}_{1}$ | -1 | t^2.523 + t^2.682 + t^2.841 + 2*t^3. + t^3.159 + t^3.318 + 3*t^4.261 + 2*t^4.42 + t^4.58 + 2*t^4.739 + t^4.898 + t^5.045 + t^5.205 + t^5.216 + 2*t^5.364 + t^5.523 + 3*t^5.682 + 2*t^5.841 - t^6. + t^6.159 + t^6.318 - t^6.477 + t^6.636 + 3*t^6.784 + 3*t^6.943 + 5*t^7.102 + 7*t^7.261 + 2*t^7.42 + t^7.568 + 4*t^7.58 + t^7.727 + 2*t^7.739 + 2*t^7.886 + 2*t^8.045 + 2*t^8.057 + 3*t^8.205 + t^8.216 + 2*t^8.364 + 3*t^8.523 + t^8.534 + 2*t^8.682 - 2*t^8.841 - t^4.42/y - t^6.943/y - t^7.102/y + t^7.739/y + t^7.898/y + t^8.205/y + t^8.364/y + (3*t^8.523)/y + (3*t^8.682)/y + (4*t^8.841)/y - t^4.42*y - t^6.943*y - t^7.102*y + t^7.739*y + t^7.898*y + t^8.205*y + t^8.364*y + 3*t^8.523*y + 3*t^8.682*y + 4*t^8.841*y | g1^6*t^2.523 + g1^4*t^2.682 + g1^2*t^2.841 + 2*t^3. + t^3.159/g1^2 + t^3.318/g1^4 + 3*g1^3*t^4.261 + 2*g1*t^4.42 + t^4.58/g1 + (2*t^4.739)/g1^3 + t^4.898/g1^5 + g1^12*t^5.045 + g1^10*t^5.205 + t^5.216/g1^9 + 2*g1^8*t^5.364 + g1^6*t^5.523 + 3*g1^4*t^5.682 + 2*g1^2*t^5.841 - t^6. + t^6.159/g1^2 + t^6.318/g1^4 - t^6.477/g1^6 + t^6.636/g1^8 + 3*g1^9*t^6.784 + 3*g1^7*t^6.943 + 5*g1^5*t^7.102 + 7*g1^3*t^7.261 + 2*g1*t^7.42 + g1^18*t^7.568 + (4*t^7.58)/g1 + g1^16*t^7.727 + (2*t^7.739)/g1^3 + 2*g1^14*t^7.886 + 2*g1^12*t^8.045 + (2*t^8.057)/g1^7 + 3*g1^10*t^8.205 + t^8.216/g1^9 + 2*g1^8*t^8.364 + 3*g1^6*t^8.523 + t^8.534/g1^13 + 2*g1^4*t^8.682 - 2*g1^2*t^8.841 - (g1*t^4.42)/y - (g1^7*t^6.943)/y - (g1^5*t^7.102)/y + t^7.739/(g1^3*y) + t^7.898/(g1^5*y) + (g1^10*t^8.205)/y + (g1^8*t^8.364)/y + (3*g1^6*t^8.523)/y + (3*g1^4*t^8.682)/y + (4*g1^2*t^8.841)/y - g1*t^4.42*y - g1^7*t^6.943*y - g1^5*t^7.102*y + (t^7.739*y)/g1^3 + (t^7.898*y)/g1^5 + g1^10*t^8.205*y + g1^8*t^8.364*y + 3*g1^6*t^8.523*y + 3*g1^4*t^8.682*y + 4*g1^2*t^8.841*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 |
|---|---|---|---|---|---|---|---|---|
| 55234 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.7046 | 0.8623 | 0.8171 | [M:[0.8626, 1.0, 1.0458, 0.9084, 1.0, 1.0458], q:[0.5229, 0.6145], qb:[0.4771, 0.4771], phi:[0.4771]] | t^2.588 + t^2.725 + 2*t^3. + 2*t^3.137 + t^3.275 + 3*t^4.294 + 2*t^4.431 + t^4.569 + 2*t^4.706 + t^4.844 + t^5.118 + t^5.176 + t^5.313 + t^5.45 + 3*t^5.725 + t^5.863 - 2*t^6. - t^4.431/y - t^4.431*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46505 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ | 0.7114 | 0.8732 | 0.8147 | [M:[0.8231, 0.9476, 1.059, 0.9345, 1.0], q:[0.5557, 0.6212], qb:[0.4967, 0.4443], phi:[0.4705]] | t^2.469 + t^2.803 + t^2.823 + t^2.843 + t^3. + t^3.177 + t^3.354 + t^4.078 + t^4.235 + t^4.392 + t^4.412 + t^4.569 + t^4.608 + t^4.746 + t^4.765 + t^4.939 + t^4.942 + t^5.139 + t^5.273 + t^5.293 + t^5.312 + t^5.607 + 3*t^5.646 + t^5.686 + t^5.823 + t^5.98 - 2*t^6. - t^4.412/y - t^4.412*y | detail |