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 |
|---|---|---|---|---|---|---|---|---|---|
| 46326 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{1}M_{3}$ | 0.6406 | 0.8108 | 0.7901 | [M:[1.1115, 0.777, 0.8885], q:[0.75, 0.473], qb:[0.3615, 0.4156], phi:[0.5]] | [M:[[-1], [2], [1]], q:[[0], [-2]], qb:[[-1], [3]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | 1 | 2*t^2.331 + t^2.503 + t^2.666 + t^3. + t^3.334 + t^3.497 + t^3.669 + t^3.831 + t^3.993 + t^4.003 + t^4.166 + t^4.338 + 3*t^4.662 + 2*t^4.834 + 2*t^4.997 + t^5.007 + t^5.169 + 3*t^5.331 + t^5.503 + 2*t^5.666 + t^5.828 + t^6. + 2*t^6.162 + 2*t^6.325 + 2*t^6.334 + 3*t^6.497 + t^6.507 + t^6.659 + 3*t^6.669 + t^6.831 + t^6.841 + 5*t^6.993 + t^7.003 + 2*t^7.166 + 3*t^7.328 + 2*t^7.338 + t^7.49 + t^7.5 + t^7.51 + 5*t^7.662 + t^7.672 + t^7.825 + 2*t^7.834 + t^7.987 + 4*t^7.997 + 2*t^8.007 + 2*t^8.159 + t^8.331 + t^8.341 + 2*t^8.493 - t^8.503 + 3*t^8.656 + t^8.675 + 4*t^8.828 + 2*t^8.99 - t^4.5/y - t^6.831/y + t^7.662/y + (2*t^7.834)/y + (2*t^7.997)/y + (2*t^8.169)/y + (2*t^8.331)/y + t^8.503/y + (3*t^8.666)/y + (2*t^8.828)/y + t^8.838/y - t^4.5*y - t^6.831*y + t^7.662*y + 2*t^7.834*y + 2*t^7.997*y + 2*t^8.169*y + 2*t^8.331*y + t^8.503*y + 3*t^8.666*y + 2*t^8.828*y + t^8.838*y | 2*g1^2*t^2.331 + t^2.503/g1^3 + g1*t^2.666 + t^3. + t^3.334/g1 + g1^3*t^3.497 + t^3.669/g1^2 + g1^2*t^3.831 + g1^6*t^3.993 + t^4.003/g1^3 + g1*t^4.166 + t^4.338/g1^4 + 3*g1^4*t^4.662 + (2*t^4.834)/g1 + 2*g1^3*t^4.997 + t^5.007/g1^6 + t^5.169/g1^2 + 3*g1^2*t^5.331 + t^5.503/g1^3 + 2*g1*t^5.666 + g1^5*t^5.828 + t^6. + 2*g1^4*t^6.162 + 2*g1^8*t^6.325 + (2*t^6.334)/g1 + 3*g1^3*t^6.497 + t^6.507/g1^6 + g1^7*t^6.659 + (3*t^6.669)/g1^2 + g1^2*t^6.831 + t^6.841/g1^7 + 5*g1^6*t^6.993 + t^7.003/g1^3 + 2*g1*t^7.166 + 3*g1^5*t^7.328 + (2*t^7.338)/g1^4 + g1^9*t^7.49 + t^7.5 + t^7.51/g1^9 + 5*g1^4*t^7.662 + t^7.672/g1^5 + g1^8*t^7.825 + (2*t^7.834)/g1 + g1^12*t^7.987 + 4*g1^3*t^7.997 + (2*t^8.007)/g1^6 + 2*g1^7*t^8.159 + g1^2*t^8.331 + t^8.341/g1^7 + 2*g1^6*t^8.493 - t^8.503/g1^3 + 3*g1^10*t^8.656 + t^8.675/g1^8 + 4*g1^5*t^8.828 + 2*g1^9*t^8.99 - t^4.5/y - (g1^2*t^6.831)/y + (g1^4*t^7.662)/y + (2*t^7.834)/(g1*y) + (2*g1^3*t^7.997)/y + (2*t^8.169)/(g1^2*y) + (2*g1^2*t^8.331)/y + t^8.503/(g1^3*y) + (3*g1*t^8.666)/y + (2*g1^5*t^8.828)/y + t^8.838/(g1^4*y) - t^4.5*y - g1^2*t^6.831*y + g1^4*t^7.662*y + (2*t^7.834*y)/g1 + 2*g1^3*t^7.997*y + (2*t^8.169*y)/g1^2 + 2*g1^2*t^8.331*y + (t^8.503*y)/g1^3 + 3*g1*t^8.666*y + 2*g1^5*t^8.828*y + (t^8.838*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46059 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ | 0.6306 | 0.7937 | 0.7946 | [M:[1.1085, 0.7829], q:[0.75, 0.4671], qb:[0.3585, 0.4244], phi:[0.5]] | 2*t^2.349 + t^2.477 + t^3. + 2*t^3.326 + t^3.523 + t^3.651 + t^3.849 + t^3.977 + t^4.047 + t^4.174 + t^4.302 + 3*t^4.698 + 2*t^4.826 + t^4.953 + 2*t^5.349 + t^5.477 + 3*t^5.674 + t^5.802 + t^5.872 - t^4.5/y - t^4.5*y | detail | {a: 895529/1420032, c: 1127041/1420032, M1: 143/129, M2: 101/129, q1: 3/4, q2: 241/516, qb1: 185/516, qb2: 73/172, phi1: 1/2} |