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 |
|---|---|---|---|---|---|---|---|---|---|
| 4871 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{2}M_{4}$ + ${ }M_{4}M_{7}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ | 0.7016 | 0.8629 | 0.813 | [M:[0.9067, 1.0467, 1.0, 0.9533, 1.0467, 0.9533, 1.0467, 0.9067], q:[0.57, 0.5233], qb:[0.43, 0.5233], phi:[0.4883]] | [M:[[-8], [4], [0], [-4], [4], [-4], [4], [-8]], q:[[6], [2]], qb:[[-6], [2]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{8}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{2}M_{8}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$ | ${}M_{2}M_{6}$, ${ }M_{6}M_{7}$ | -3 | 2*t^2.72 + t^2.86 + t^2.93 + t^3. + 2*t^3.14 + t^4.045 + 2*t^4.325 + t^4.465 + 3*t^4.605 + 2*t^4.745 + t^4.885 + 3*t^5.44 + t^5.58 + 2*t^5.65 + t^5.72 + t^5.79 + 4*t^5.86 + t^5.93 - 3*t^6. + 2*t^6.07 - t^6.14 + t^6.28 - t^6.42 + 2*t^6.765 + t^6.905 + t^6.975 + 4*t^7.045 - t^7.115 + 3*t^7.185 + 2*t^7.255 + 5*t^7.325 - t^7.395 + 5*t^7.465 + 2*t^7.535 + 2*t^7.605 - t^7.675 + 5*t^7.745 - t^7.815 + 2*t^7.885 - t^7.955 + t^8.025 + t^8.09 + 4*t^8.16 + t^8.3 + 5*t^8.37 + 2*t^8.51 + 5*t^8.58 + 4*t^8.65 - 7*t^8.72 + 6*t^8.79 - 5*t^8.86 + 2*t^8.93 - t^4.465/y - (2*t^7.185)/y + t^7.325/y - t^7.395/y + t^7.535/y - t^7.605/y + (2*t^7.745)/y + t^8.44/y + (2*t^8.58)/y + (2*t^8.65)/y + (2*t^8.72)/y + t^8.79/y + (5*t^8.86)/y + t^8.93/y - t^4.465*y - 2*t^7.185*y + t^7.325*y - t^7.395*y + t^7.535*y - t^7.605*y + 2*t^7.745*y + t^8.44*y + 2*t^8.58*y + 2*t^8.65*y + 2*t^8.72*y + t^8.79*y + 5*t^8.86*y + t^8.93*y | (2*t^2.72)/g1^8 + t^2.86/g1^4 + t^2.93/g1^2 + t^3. + 2*g1^4*t^3.14 + t^4.045/g1^13 + (2*t^4.325)/g1^5 + t^4.465/g1 + 3*g1^3*t^4.605 + 2*g1^7*t^4.745 + g1^11*t^4.885 + (3*t^5.44)/g1^16 + t^5.58/g1^12 + (2*t^5.65)/g1^10 + t^5.72/g1^8 + t^5.79/g1^6 + (4*t^5.86)/g1^4 + t^5.93/g1^2 - 3*t^6. + 2*g1^2*t^6.07 - g1^4*t^6.14 + g1^8*t^6.28 - g1^12*t^6.42 + (2*t^6.765)/g1^21 + t^6.905/g1^17 + t^6.975/g1^15 + (4*t^7.045)/g1^13 - t^7.115/g1^11 + (3*t^7.185)/g1^9 + (2*t^7.255)/g1^7 + (5*t^7.325)/g1^5 - t^7.395/g1^3 + (5*t^7.465)/g1 + 2*g1*t^7.535 + 2*g1^3*t^7.605 - g1^5*t^7.675 + 5*g1^7*t^7.745 - g1^9*t^7.815 + 2*g1^11*t^7.885 - g1^13*t^7.955 + g1^15*t^8.025 + t^8.09/g1^26 + (4*t^8.16)/g1^24 + t^8.3/g1^20 + (5*t^8.37)/g1^18 + (2*t^8.51)/g1^14 + (5*t^8.58)/g1^12 + (4*t^8.65)/g1^10 - (7*t^8.72)/g1^8 + (6*t^8.79)/g1^6 - (5*t^8.86)/g1^4 + (2*t^8.93)/g1^2 - t^4.465/(g1*y) - (2*t^7.185)/(g1^9*y) + t^7.325/(g1^5*y) - t^7.395/(g1^3*y) + (g1*t^7.535)/y - (g1^3*t^7.605)/y + (2*g1^7*t^7.745)/y + t^8.44/(g1^16*y) + (2*t^8.58)/(g1^12*y) + (2*t^8.65)/(g1^10*y) + (2*t^8.72)/(g1^8*y) + t^8.79/(g1^6*y) + (5*t^8.86)/(g1^4*y) + t^8.93/(g1^2*y) - (t^4.465*y)/g1 - (2*t^7.185*y)/g1^9 + (t^7.325*y)/g1^5 - (t^7.395*y)/g1^3 + g1*t^7.535*y - g1^3*t^7.605*y + 2*g1^7*t^7.745*y + (t^8.44*y)/g1^16 + (2*t^8.58*y)/g1^12 + (2*t^8.65*y)/g1^10 + (2*t^8.72*y)/g1^8 + (t^8.79*y)/g1^6 + (5*t^8.86*y)/g1^4 + (t^8.93*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2683 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{2}M_{4}$ + ${ }M_{4}M_{7}$ | 0.6947 | 0.8505 | 0.8168 | [M:[0.9451, 1.0275, 1.0, 0.9725, 1.0275, 0.9725, 1.0275], q:[0.5412, 0.5137], qb:[0.4588, 0.5137], phi:[0.4931]] | t^2.835 + t^2.918 + t^2.959 + t^3. + 2*t^3.082 + t^3.165 + t^4.232 + 2*t^4.397 + t^4.479 + 3*t^4.562 + 2*t^4.644 + t^4.727 + t^5.67 + t^5.794 + t^5.876 + 2*t^5.918 + t^5.959 - 2*t^6. - t^4.479/y - t^4.479*y | detail |