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 |
|---|---|---|---|---|---|---|---|---|---|
| 48106 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ + ${ }M_{3}M_{5}$ | 0.7002 | 0.8574 | 0.8166 | [M:[0.9692, 0.9384, 1.0616, 1.0, 0.9384], q:[0.5462, 0.4846], qb:[0.577, 0.4538], phi:[0.4846]] | [M:[[2], [4], [-4], [0], [4]], q:[[-3], [1]], qb:[[-5], [3]], phi:[[1]]] |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | 2*t^2.815 + 2*t^2.908 + t^3. + t^3.092 + t^3.37 + t^4.176 + t^4.269 + t^4.361 + t^4.454 + 2*t^4.546 + t^4.639 + t^4.731 + t^4.824 + t^4.916 + 2*t^5.63 + 2*t^5.723 + 4*t^5.815 + 2*t^5.908 - t^6. - t^6.092 + t^6.185 + t^6.462 + t^6.74 + 2*t^6.992 + 3*t^7.084 + 3*t^7.176 + 3*t^7.269 + 3*t^7.361 + 3*t^7.454 + 3*t^7.546 + 2*t^7.639 + 2*t^7.731 + 2*t^7.824 + t^7.916 + t^8.101 + t^8.193 + t^8.286 + t^8.353 + 3*t^8.445 + 2*t^8.538 + 5*t^8.63 + 7*t^8.723 - 2*t^8.815 - 2*t^8.908 - t^4.454/y - t^7.269/y - (2*t^7.361)/y + (2*t^7.546)/y + t^7.639/y + t^8.63/y + (4*t^8.723)/y + (3*t^8.815)/y + (4*t^8.908)/y - t^4.454*y - t^7.269*y - 2*t^7.361*y + 2*t^7.546*y + t^7.639*y + t^8.63*y + 4*t^8.723*y + 3*t^8.815*y + 4*t^8.908*y | 2*g1^4*t^2.815 + 2*g1^2*t^2.908 + t^3. + t^3.092/g1^2 + t^3.37/g1^8 + g1^7*t^4.176 + g1^5*t^4.269 + g1^3*t^4.361 + g1*t^4.454 + (2*t^4.546)/g1 + t^4.639/g1^3 + t^4.731/g1^5 + t^4.824/g1^7 + t^4.916/g1^9 + 2*g1^8*t^5.63 + 2*g1^6*t^5.723 + 4*g1^4*t^5.815 + 2*g1^2*t^5.908 - t^6. - t^6.092/g1^2 + t^6.185/g1^4 + t^6.462/g1^10 + t^6.74/g1^16 + 2*g1^11*t^6.992 + 3*g1^9*t^7.084 + 3*g1^7*t^7.176 + 3*g1^5*t^7.269 + 3*g1^3*t^7.361 + 3*g1*t^7.454 + (3*t^7.546)/g1 + (2*t^7.639)/g1^3 + (2*t^7.731)/g1^5 + (2*t^7.824)/g1^7 + t^7.916/g1^9 + t^8.101/g1^13 + t^8.193/g1^15 + t^8.286/g1^17 + g1^14*t^8.353 + 3*g1^12*t^8.445 + 2*g1^10*t^8.538 + 5*g1^8*t^8.63 + 7*g1^6*t^8.723 - 2*g1^4*t^8.815 - 2*g1^2*t^8.908 - (g1*t^4.454)/y - (g1^5*t^7.269)/y - (2*g1^3*t^7.361)/y + (2*t^7.546)/(g1*y) + t^7.639/(g1^3*y) + (g1^8*t^8.63)/y + (4*g1^6*t^8.723)/y + (3*g1^4*t^8.815)/y + (4*g1^2*t^8.908)/y - g1*t^4.454*y - g1^5*t^7.269*y - 2*g1^3*t^7.361*y + (2*t^7.546*y)/g1 + (t^7.639*y)/g1^3 + g1^8*t^8.63*y + 4*g1^6*t^8.723*y + 3*g1^4*t^8.815*y + 4*g1^2*t^8.908*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 |
|---|---|---|---|---|---|---|---|---|
| 53432 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | 0.7033 | 0.8629 | 0.815 | [M:[0.964, 0.9281, 1.0719, 1.0, 0.9281, 0.964], q:[0.554, 0.482], qb:[0.5899, 0.446], phi:[0.482]] | 2*t^2.784 + 3*t^2.892 + t^3. + t^3.432 + t^4.122 + t^4.23 + t^4.338 + t^4.446 + 2*t^4.554 + t^4.662 + t^4.77 + t^4.878 + t^4.986 + 2*t^5.568 + 4*t^5.676 + 7*t^5.784 + t^5.892 - 3*t^6. - t^4.446/y - t^4.446*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46720 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ | 0.6954 | 0.8497 | 0.8184 | [M:[0.9793, 0.9586, 1.0414, 1.0], q:[0.5311, 0.4896], qb:[0.5518, 0.4689], phi:[0.4896]] | t^2.876 + 2*t^2.938 + t^3. + t^3.062 + t^3.124 + t^3.248 + t^4.283 + t^4.345 + t^4.407 + t^4.469 + 2*t^4.531 + t^4.593 + t^4.655 + t^4.717 + t^4.78 + 3*t^5.876 + t^5.938 - t^4.469/y - t^4.469*y | detail |