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 |
---|---|---|---|---|---|---|---|---|---|
1833 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{1}q_{2}$ | 0.6586 | 0.8461 | 0.7784 | [M:[1.1497, 1.1497, 0.7005, 0.7005, 0.7995], q:[0.75, 0.4505], qb:[0.3997, 0.3997], phi:[0.5]] | [M:[[1], [1], [-2], [-2], [2]], q:[[0], [-2]], qb:[[1], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{4}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{5}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{4}\phi_{1}\tilde{q}_{2}^{2}$ | -3 | 2*t^2.102 + 2*t^2.398 + t^3. + 4*t^3.449 + t^3.898 + 2*t^4.051 + 4*t^4.203 + 4*t^4.5 + 3*t^4.797 + 2*t^5.102 + 2*t^5.398 + 8*t^5.551 + 6*t^5.848 - 3*t^6. + 2*t^6.152 + 2*t^6.297 + 6*t^6.305 + 4*t^6.449 + 6*t^6.602 + 13*t^6.898 - 2*t^7.051 + 4*t^7.195 + 3*t^7.203 + 4*t^7.5 + 12*t^7.652 + 3*t^7.797 + 10*t^7.949 - 7*t^8.102 + 8*t^8.246 + 4*t^8.254 - 6*t^8.398 + 9*t^8.406 + 4*t^8.551 + 3*t^8.695 + 8*t^8.703 + 4*t^8.848 - t^4.5/y - (2*t^6.602)/y - t^6.898/y + (2*t^7.051)/y + t^7.203/y + (4*t^7.5)/y + t^7.797/y - (2*t^7.949)/y + (3*t^8.102)/y + (4*t^8.398)/y + (8*t^8.551)/y - (3*t^8.703)/y + (8*t^8.848)/y - t^4.5*y - 2*t^6.602*y - t^6.898*y + 2*t^7.051*y + t^7.203*y + 4*t^7.5*y + t^7.797*y - 2*t^7.949*y + 3*t^8.102*y + 4*t^8.398*y + 8*t^8.551*y - 3*t^8.703*y + 8*t^8.848*y | (2*t^2.102)/g1^2 + 2*g1^2*t^2.398 + t^3. + 4*g1*t^3.449 + g1^2*t^3.898 + (2*t^4.051)/g1 + (4*t^4.203)/g1^4 + 4*t^4.5 + 3*g1^4*t^4.797 + (2*t^5.102)/g1^2 + 2*g1^2*t^5.398 + (8*t^5.551)/g1 + 6*g1^3*t^5.848 - 3*t^6. + (2*t^6.152)/g1^3 + 2*g1^4*t^6.297 + (6*t^6.305)/g1^6 + 4*g1*t^6.449 + (6*t^6.602)/g1^2 + 13*g1^2*t^6.898 - (2*t^7.051)/g1 + 4*g1^6*t^7.195 + (3*t^7.203)/g1^4 + 4*t^7.5 + (12*t^7.652)/g1^3 + 3*g1^4*t^7.797 + 10*g1*t^7.949 - (7*t^8.102)/g1^2 + 8*g1^5*t^8.246 + (4*t^8.254)/g1^5 - 6*g1^2*t^8.398 + (9*t^8.406)/g1^8 + (4*t^8.551)/g1 + 3*g1^6*t^8.695 + (8*t^8.703)/g1^4 + 4*g1^3*t^8.848 - t^4.5/y - (2*t^6.602)/(g1^2*y) - (g1^2*t^6.898)/y + (2*t^7.051)/(g1*y) + t^7.203/(g1^4*y) + (4*t^7.5)/y + (g1^4*t^7.797)/y - (2*g1*t^7.949)/y + (3*t^8.102)/(g1^2*y) + (4*g1^2*t^8.398)/y + (8*t^8.551)/(g1*y) - (3*t^8.703)/(g1^4*y) + (8*g1^3*t^8.848)/y - t^4.5*y - (2*t^6.602*y)/g1^2 - g1^2*t^6.898*y + (2*t^7.051*y)/g1 + (t^7.203*y)/g1^4 + 4*t^7.5*y + g1^4*t^7.797*y - 2*g1*t^7.949*y + (3*t^8.102*y)/g1^2 + 4*g1^2*t^8.398*y + (8*t^8.551*y)/g1 - (3*t^8.703*y)/g1^4 + 8*g1^3*t^8.848*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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
392 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6426 | 0.8185 | 0.785 | [M:[1.1576, 1.1576, 0.6848, 0.6848], q:[0.75, 0.4348], qb:[0.4076, 0.4076], phi:[0.5]] | 2*t^2.054 + t^2.446 + t^3. + 4*t^3.473 + t^3.554 + t^3.946 + 2*t^4.027 + 4*t^4.109 + 2*t^4.5 + t^4.891 + 2*t^5.054 + t^5.446 + 8*t^5.527 + 2*t^5.609 + 2*t^5.919 - 2*t^6. - t^4.5/y - t^4.5*y | detail |