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 |
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2565 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}M_{7}$ | 0.6944 | 0.8518 | 0.8152 | [M:[0.9768, 1.0077, 1.0232, 0.9613, 1.0387, 0.9923, 0.9613], q:[0.5193, 0.5039], qb:[0.4574, 0.5348], phi:[0.4961]] | [M:[[-6], [2], [6], [-10], [10], [-2], [-10]], q:[[5], [1]], qb:[[-11], [9]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -3 | 2*t^2.884 + t^2.93 + 2*t^2.977 + t^3.07 + t^3.163 + t^4.233 + t^4.372 + t^4.419 + t^4.465 + t^4.512 + t^4.558 + 2*t^4.604 + t^4.651 + t^4.697 + 2*t^5.768 + t^5.814 + 4*t^5.861 + t^5.907 + 3*t^5.954 - 3*t^6. + t^6.046 + 2*t^6.139 - t^6.186 + t^6.325 + 2*t^7.117 + t^7.163 + 2*t^7.21 + 2*t^7.303 + 3*t^7.349 + 3*t^7.396 + 2*t^7.442 + 2*t^7.488 + 2*t^7.535 + 5*t^7.581 + t^7.628 + 2*t^7.674 - t^7.721 + 2*t^7.767 + t^7.813 + t^7.86 + t^8.466 + t^8.605 + 3*t^8.652 + t^8.698 + 4*t^8.745 + 2*t^8.791 + 7*t^8.837 - 3*t^8.884 + t^8.93 - 7*t^8.977 - t^4.488/y - t^7.372/y - t^7.465/y + t^7.512/y + t^7.604/y + t^8.768/y + (2*t^8.814)/y + (4*t^8.861)/y + (2*t^8.907)/y + (3*t^8.954)/y - t^4.488*y - t^7.372*y - t^7.465*y + t^7.512*y + t^7.604*y + t^8.768*y + 2*t^8.814*y + 4*t^8.861*y + 2*t^8.907*y + 3*t^8.954*y | (2*t^2.884)/g1^10 + t^2.93/g1^6 + (2*t^2.977)/g1^2 + g1^6*t^3.07 + g1^14*t^3.163 + t^4.233/g1^23 + t^4.372/g1^11 + t^4.419/g1^7 + t^4.465/g1^3 + g1*t^4.512 + g1^5*t^4.558 + 2*g1^9*t^4.604 + g1^13*t^4.651 + g1^17*t^4.697 + (2*t^5.768)/g1^20 + t^5.814/g1^16 + (4*t^5.861)/g1^12 + t^5.907/g1^8 + (3*t^5.954)/g1^4 - 3*t^6. + g1^4*t^6.046 + 2*g1^12*t^6.139 - g1^16*t^6.186 + g1^28*t^6.325 + (2*t^7.117)/g1^33 + t^7.163/g1^29 + (2*t^7.21)/g1^25 + (2*t^7.303)/g1^17 + (3*t^7.349)/g1^13 + (3*t^7.396)/g1^9 + (2*t^7.442)/g1^5 + (2*t^7.488)/g1 + 2*g1^3*t^7.535 + 5*g1^7*t^7.581 + g1^11*t^7.628 + 2*g1^15*t^7.674 - g1^19*t^7.721 + 2*g1^23*t^7.767 + g1^27*t^7.813 + g1^31*t^7.86 + t^8.466/g1^46 + t^8.605/g1^34 + (3*t^8.652)/g1^30 + t^8.698/g1^26 + (4*t^8.745)/g1^22 + (2*t^8.791)/g1^18 + (7*t^8.837)/g1^14 - (3*t^8.884)/g1^10 + t^8.93/g1^6 - (7*t^8.977)/g1^2 - t^4.488/(g1*y) - t^7.372/(g1^11*y) - t^7.465/(g1^3*y) + (g1*t^7.512)/y + (g1^9*t^7.604)/y + t^8.768/(g1^20*y) + (2*t^8.814)/(g1^16*y) + (4*t^8.861)/(g1^12*y) + (2*t^8.907)/(g1^8*y) + (3*t^8.954)/(g1^4*y) - (t^4.488*y)/g1 - (t^7.372*y)/g1^11 - (t^7.465*y)/g1^3 + g1*t^7.512*y + g1^9*t^7.604*y + (t^8.768*y)/g1^20 + (2*t^8.814*y)/g1^16 + (4*t^8.861*y)/g1^12 + (2*t^8.907*y)/g1^8 + (3*t^8.954*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 |
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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 |
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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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
1486 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{6}$ | 0.6918 | 0.8476 | 0.8162 | [M:[0.991, 1.003, 1.009, 0.9849, 1.0151, 0.997], q:[0.5075, 0.5015], qb:[0.4834, 0.5136], phi:[0.4985]] | t^2.955 + t^2.973 + 2*t^2.991 + t^3.027 + t^3.045 + t^3.063 + t^4.396 + t^4.45 + t^4.468 + t^4.486 + t^4.505 + t^4.523 + 2*t^4.541 + t^4.559 + t^4.577 + 2*t^5.946 + t^5.964 + 2*t^5.982 - 2*t^6. - t^4.495/y - t^4.495*y | detail |