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 |
|---|---|---|---|---|---|---|---|---|---|
| 965 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}^{2}$ + ${ }M_{3}M_{6}$ | 0.7077 | 0.8618 | 0.8212 | [M:[0.8615, 1.0, 0.8615, 1.0, 1.0, 1.1385], q:[0.6385, 0.5], qb:[0.5, 0.5], phi:[0.4654]] | [M:[[-4, 0], [0, 0], [-4, 1], [0, -1], [0, 1], [4, -1]], q:[[4, 0], [0, 0]], qb:[[0, -1], [0, 1]], phi:[[-1, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$ | -2 | t^2.584 + t^2.792 + 3*t^3. + 2*t^3.416 + 6*t^4.396 + 3*t^4.812 + t^5.169 + t^5.227 + t^5.377 + t^5.584 + 3*t^5.792 - 2*t^6. + 2*t^6.208 + 2*t^6.416 + 3*t^6.831 + 3*t^6.981 + 6*t^7.188 + 9*t^7.396 - 3*t^7.604 + t^7.753 + 10*t^7.812 + t^7.961 - 2*t^8.019 + 2*t^8.169 + 6*t^8.227 + t^8.377 - t^8.435 - 4*t^8.584 + 2*t^8.643 + 13*t^8.792 - t^4.396/y - t^6.981/y - t^7.188/y + t^7.604/y + t^7.812/y + t^8.377/y + (3*t^8.584)/y + (3*t^8.792)/y - t^4.396*y - t^6.981*y - t^7.188*y + t^7.604*y + t^7.812*y + t^8.377*y + 3*t^8.584*y + 3*t^8.792*y | t^2.584/g1^4 + t^2.792/g1^2 + t^3. + t^3./g2 + g2*t^3. + (g1^4*t^3.416)/g2 + g1^4*g2*t^3.416 + (2*t^4.396)/g1 + t^4.396/(g1*g2^2) + t^4.396/(g1*g2) + (g2*t^4.396)/g1 + (g2^2*t^4.396)/g1 + g1^3*t^4.812 + (g1^3*t^4.812)/g2 + g1^3*g2*t^4.812 + t^5.169/g1^8 + g1^7*t^5.227 + t^5.377/g1^6 + t^5.584/g1^4 + t^5.792/g1^2 + t^5.792/(g1^2*g2) + (g2*t^5.792)/g1^2 - 2*t^6. + (g1^2*t^6.208)/g2 + g1^2*g2*t^6.208 + (g1^4*t^6.416)/g2^2 + g1^4*g2^2*t^6.416 + g1^8*t^6.831 + (g1^8*t^6.831)/g2^2 + g1^8*g2^2*t^6.831 + t^6.981/g1^5 + t^6.981/(g1^5*g2^2) + (g2^2*t^6.981)/g1^5 + (2*t^7.188)/g1^3 + t^7.188/(g1^3*g2^2) + t^7.188/(g1^3*g2) + (g2*t^7.188)/g1^3 + (g2^2*t^7.188)/g1^3 + t^7.396/g1 + t^7.396/(g1*g2^3) + t^7.396/(g1*g2^2) + (2*t^7.396)/(g1*g2) + (2*g2*t^7.396)/g1 + (g2^2*t^7.396)/g1 + (g2^3*t^7.396)/g1 - g1*t^7.604 - (g1*t^7.604)/g2^2 - g1*g2^2*t^7.604 + t^7.753/g1^12 + 2*g1^3*t^7.812 + (g1^3*t^7.812)/g2^3 + (g1^3*t^7.812)/g2^2 + (2*g1^3*t^7.812)/g2 + 2*g1^3*g2*t^7.812 + g1^3*g2^2*t^7.812 + g1^3*g2^3*t^7.812 + t^7.961/g1^10 - (g1^5*t^8.019)/g2 - g1^5*g2*t^8.019 + (2*t^8.169)/g1^8 + 2*g1^7*t^8.227 + (g1^7*t^8.227)/g2^2 + (g1^7*t^8.227)/g2 + g1^7*g2*t^8.227 + g1^7*g2^2*t^8.227 + t^8.377/g1^6 - g1^9*t^8.435 - (2*t^8.584)/g1^4 - t^8.584/(g1^4*g2^2) - (g2^2*t^8.584)/g1^4 + (g1^11*t^8.643)/g2 + g1^11*g2*t^8.643 + t^8.792/g1^2 + t^8.792/(g1^2*g2^4) + t^8.792/(g1^2*g2^3) + (2*t^8.792)/(g1^2*g2^2) + (2*t^8.792)/(g1^2*g2) + (2*g2*t^8.792)/g1^2 + (2*g2^2*t^8.792)/g1^2 + (g2^3*t^8.792)/g1^2 + (g2^4*t^8.792)/g1^2 - t^4.396/(g1*y) - t^6.981/(g1^5*y) - t^7.188/(g1^3*y) + (g1*t^7.604)/y + (g1^3*t^7.812)/y + t^8.377/(g1^6*y) + t^8.584/(g1^4*y) + t^8.584/(g1^4*g2*y) + (g2*t^8.584)/(g1^4*y) + t^8.792/(g1^2*y) + t^8.792/(g1^2*g2*y) + (g2*t^8.792)/(g1^2*y) - (t^4.396*y)/g1 - (t^6.981*y)/g1^5 - (t^7.188*y)/g1^3 + g1*t^7.604*y + g1^3*t^7.812*y + (t^8.377*y)/g1^6 + (t^8.584*y)/g1^4 + (t^8.584*y)/(g1^4*g2) + (g2*t^8.584*y)/g1^4 + (t^8.792*y)/g1^2 + (t^8.792*y)/(g1^2*g2) + (g2*t^8.792*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 |
|---|---|---|---|---|---|---|---|---|---|
| 601 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}^{2}$ | 0.7222 | 0.8878 | 0.8134 | [M:[0.8228, 1.0, 0.8046, 1.0182, 0.9818], q:[0.6772, 0.5], qb:[0.5182, 0.4818], phi:[0.4557]] | t^2.414 + t^2.468 + t^2.734 + t^2.945 + t^3. + t^3.055 + t^3.477 + t^4.258 + t^4.312 + 2*t^4.367 + t^4.422 + t^4.477 + t^4.828 + t^4.844 + t^4.882 + t^4.899 + t^4.937 + t^4.953 + t^5.148 + t^5.203 + t^5.359 + t^5.414 + t^5.43 + 2*t^5.468 + t^5.68 + t^5.734 + t^5.789 + t^5.891 - 2*t^6. - t^4.367/y - t^4.367*y | detail |