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 |
---|---|---|---|---|---|---|---|---|---|
46486 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6691 | 0.8669 | 0.7718 | [M:[1.1117, 0.7765, 0.7765, 0.6704], q:[0.75, 0.4735], qb:[0.3617, 0.4148], phi:[0.5]] | [M:[[-1], [2], [2], [-6]], q:[[0], [-2]], qb:[[-1], [3]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.011 + 3*t^2.33 + t^2.506 + t^3. + 2*t^3.335 + t^3.494 + t^3.83 + t^4.006 + t^4.023 + t^4.165 + 4*t^4.341 + t^4.517 + 6*t^4.659 + 3*t^4.835 + 2*t^5.011 + 3*t^5.33 + 2*t^5.346 + 2*t^5.506 + 5*t^5.665 + 2*t^5.824 + 2*t^5.841 - 2*t^6. + t^6.017 + t^6.034 + 2*t^6.159 + 3*t^6.335 + 4*t^6.352 + 2*t^6.494 + t^6.511 + t^6.528 + 10*t^6.67 + t^6.83 + 4*t^6.846 + 10*t^6.989 - t^7.006 + 2*t^7.023 + 5*t^7.165 - t^7.324 + 6*t^7.341 + 2*t^7.358 - t^7.5 + 3*t^7.517 + 5*t^7.659 + 5*t^7.676 + 3*t^7.835 + 2*t^7.852 + 8*t^7.994 - t^8.011 + t^8.028 + t^8.045 + 3*t^8.154 + 4*t^8.17 - 7*t^8.33 + 5*t^8.346 + 4*t^8.363 + 3*t^8.489 - 2*t^8.506 + t^8.523 + t^8.539 + 4*t^8.665 + 10*t^8.682 + 2*t^8.824 + 3*t^8.841 + 4*t^8.858 - t^4.5/y - t^6.511/y - (2*t^6.83)/y + t^7.165/y + (3*t^7.341)/y + t^7.517/y + (3*t^7.659)/y + (2*t^7.835)/y + t^8.011/y + (2*t^8.17)/y + (3*t^8.33)/y + (2*t^8.346)/y + t^8.489/y + (2*t^8.506)/y - t^8.523/y + (6*t^8.665)/y + (3*t^8.824)/y + t^8.841/y - t^4.5*y - t^6.511*y - 2*t^6.83*y + t^7.165*y + 3*t^7.341*y + t^7.517*y + 3*t^7.659*y + 2*t^7.835*y + t^8.011*y + 2*t^8.17*y + 3*t^8.33*y + 2*t^8.346*y + t^8.489*y + 2*t^8.506*y - t^8.523*y + 6*t^8.665*y + 3*t^8.824*y + t^8.841*y | t^2.011/g1^6 + 3*g1^2*t^2.33 + t^2.506/g1^3 + t^3. + (2*t^3.335)/g1 + g1^3*t^3.494 + g1^2*t^3.83 + t^4.006/g1^3 + t^4.023/g1^12 + g1*t^4.165 + (4*t^4.341)/g1^4 + t^4.517/g1^9 + 6*g1^4*t^4.659 + (3*t^4.835)/g1 + (2*t^5.011)/g1^6 + 3*g1^2*t^5.33 + (2*t^5.346)/g1^7 + (2*t^5.506)/g1^3 + 5*g1*t^5.665 + 2*g1^5*t^5.824 + (2*t^5.841)/g1^4 - 2*t^6. + t^6.017/g1^9 + t^6.034/g1^18 + 2*g1^4*t^6.159 + (3*t^6.335)/g1 + (4*t^6.352)/g1^10 + 2*g1^3*t^6.494 + t^6.511/g1^6 + t^6.528/g1^15 + (10*t^6.67)/g1^2 + g1^2*t^6.83 + (4*t^6.846)/g1^7 + 10*g1^6*t^6.989 - t^7.006/g1^3 + (2*t^7.023)/g1^12 + 5*g1*t^7.165 - g1^5*t^7.324 + (6*t^7.341)/g1^4 + (2*t^7.358)/g1^13 - t^7.5 + (3*t^7.517)/g1^9 + 5*g1^4*t^7.659 + (5*t^7.676)/g1^5 + (3*t^7.835)/g1 + (2*t^7.852)/g1^10 + 8*g1^3*t^7.994 - t^8.011/g1^6 + t^8.028/g1^15 + t^8.045/g1^24 + 3*g1^7*t^8.154 + (4*t^8.17)/g1^2 - 7*g1^2*t^8.33 + (5*t^8.346)/g1^7 + (4*t^8.363)/g1^16 + 3*g1^6*t^8.489 - (2*t^8.506)/g1^3 + t^8.523/g1^12 + t^8.539/g1^21 + 4*g1*t^8.665 + (10*t^8.682)/g1^8 + 2*g1^5*t^8.824 + (3*t^8.841)/g1^4 + (4*t^8.858)/g1^13 - t^4.5/y - t^6.511/(g1^6*y) - (2*g1^2*t^6.83)/y + (g1*t^7.165)/y + (3*t^7.341)/(g1^4*y) + t^7.517/(g1^9*y) + (3*g1^4*t^7.659)/y + (2*t^7.835)/(g1*y) + t^8.011/(g1^6*y) + (2*t^8.17)/(g1^2*y) + (3*g1^2*t^8.33)/y + (2*t^8.346)/(g1^7*y) + (g1^6*t^8.489)/y + (2*t^8.506)/(g1^3*y) - t^8.523/(g1^12*y) + (6*g1*t^8.665)/y + (3*g1^5*t^8.824)/y + t^8.841/(g1^4*y) - t^4.5*y - (t^6.511*y)/g1^6 - 2*g1^2*t^6.83*y + g1*t^7.165*y + (3*t^7.341*y)/g1^4 + (t^7.517*y)/g1^9 + 3*g1^4*t^7.659*y + (2*t^7.835*y)/g1 + (t^8.011*y)/g1^6 + (2*t^8.17*y)/g1^2 + 3*g1^2*t^8.33*y + (2*t^8.346*y)/g1^7 + g1^6*t^8.489*y + (2*t^8.506*y)/g1^3 - (t^8.523*y)/g1^12 + 6*g1*t^8.665*y + 3*g1^5*t^8.824*y + (t^8.841*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 |
---|---|---|---|---|---|---|---|---|
48139 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6464 | 0.8383 | 0.771 | [M:[1.1429, 0.7143, 0.7143, 0.8571], q:[0.75, 0.5357], qb:[0.3929, 0.3214], phi:[0.5]] | 3*t^2.143 + t^2.571 + t^2.786 + t^3. + t^3.214 + 2*t^3.429 + t^3.643 + t^4.071 + 7*t^4.286 + 4*t^4.714 + 3*t^4.929 + 4*t^5.143 + 3*t^5.357 + 7*t^5.571 + 4*t^5.786 - t^4.5/y - t^4.5*y | detail | {a: 56757/87808, c: 73613/87808, M1: 8/7, M2: 5/7, M3: 5/7, M4: 6/7, q1: 3/4, q2: 15/28, qb1: 11/28, qb2: 9/28, phi1: 1/2} |
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 |
---|---|---|---|---|---|---|---|---|---|
46215 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}q_{1}q_{2}$ | 0.6483 | 0.8256 | 0.7853 | [M:[1.1122, 0.7757, 0.7757], q:[0.75, 0.4743], qb:[0.3622, 0.4135], phi:[0.5]] | 3*t^2.327 + t^2.509 + t^3. + 2*t^3.336 + t^3.491 + t^3.827 + t^3.981 + t^4.009 + t^4.164 + t^4.346 + 6*t^4.654 + 3*t^4.836 + t^5.019 + 3*t^5.327 + t^5.509 + 5*t^5.664 + 2*t^5.818 + t^5.846 - 2*t^6. - t^4.5/y - t^4.5*y | detail |